ON THE ARGUMENT OF ABEL. William Rowan Hamilton

Size: px
Start display at page:

Download "ON THE ARGUMENT OF ABEL. William Rowan Hamilton"

Transcription

1 ON THE ARGUMENT OF ABEL By Wllam Rowan Hamlton (Transactons of the Royal Irsh Academy, 8 (839), pp ) Edted by Davd R. Wlkns 2000

2 NOTE ON THE TEXT The text of ths edton s taken from the 8th volume of the Transactons of the Royal Irsh Academy. A small number of obvous typographcal errors have been corrected wthout comment n artcles, 3, 5, 6, 0 and 2. Davd R. Wlkns Dubln, February 2000

3 On the Argument of Abel, respectng the Impossblty of expressng a Root of any General Equaton above the Fourth Degree, by any fnte Combnaton of Radcals and Ratonal Functons. By Sr Wllam Rowan Hamlton. Read 22nd May, 837. [Transactons of the Royal Irsh Academy, vol. xv (839), pp ] [.] Let a, a 2,... a n be any n arbtrary quanttes, or ndependent varables, real or magnary, and let a, a 2,... a n be any n radcals, such that a α = f (a,... a n ),... a α n n = f n (a,... a n ); agan, let a,... a n be n new radcals, such that a α = f (a,... a n, a,... a n ), a α n n = f n (a,... a n, a,... a n ); and so on, tll we arrve at a system of equatons of the form a (m)α(m) = f (m ) (a (m ),... a (m ), a (m 2) n (m ),... a (m 2),... a n (m 2),... a n ), a (m)α(m) n (m) n (m) = f (m ) (a (m ) n (m),... a (m ), a (m 2) n (m ),... a (m 2),... a n (m 2),... a n ), the exponents α (k) beng all ntegral and prme numbers greater than unty, and the functons f (k ) beng ratonal, but all beng otherwse arbtrary. Then, f we represent by b (m) any ratonal functon f (m) of all the foregong quanttes a (k), b (m) = f (m) (a (m),... a (m) n (m), a (m ),... a (m ) n (m ),... a,... a n ), we may consder the quantty b (m) as beng also an rratonal functon of the n orgnal quanttes, a,... a n ; n whch latter vew t may be sad, accordng to a phraseology proposed by Abel, to be an rratonal functon of the m th order: and may be regarded as the general type of every concevable functon of any fnte number of ndependent varables, whch can be formed by any fnte number of addtons, subtractons, multplcatons, dvsons, elevatons

4 to powers, and extracton of roots of functons; snce t s obvous that any extracton of a radcal wth a composte exponent, such as α 2 α f, may be reduced to a system of successve extractons of radcals wth prme exponents, such as α f = f, α 2 f = f. Insomuch that the queston, Whether t be possble to express a root x of the general equaton of the n th degree, x n + a x n + + a n x + a n = 0, n terms of the coeffcents of that equaton, by any fnte combnaton of radcals and ratonal functons?, s, as Abel has remarked, equvalent to the queston, Whether t be possble to equate a root of the general equaton of any gven degree to an rratonal functon of the coeffcents of that equaton, whch functon shall be of any fnte order m? or to ths other queston: Is t possble to satsfy, by any functon of the form b (m), the equaton b (m)n + a b (m)n + + a n b (m) + a n = 0, n whch the exponent n s gven, but the coeffcents a, a 2,... a n are arbtrary? [2.] For the cases n = 2, n = 3, n = 4, ths queston has long snce been determned n the affrmatve, by the dscovery of the known solutons of the general quadratc, cubc, and bquadratc equatons. Thus, for n = 2, t has long been known that a root x of the general quadratc equaton, x 2 + a x + a 2 = 0, can be expressed as a fnte rratonal functon of the two arbtrary coeffcents a, a 2, namely, as the followng functon, whch s of the frst order: the radcal a beng such that x = b = f (a, a, a 2 ) = a 2 + a, a 2 = f (a, a 2 ) = a2 4 a 2; nsomuch that, wth ths form of the rratonal functon b, the equaton b 2 + a b + a 2 = 0 s satsfed, ndependently of the quanttes a and a 2, whch reman altogether arbtrary. Agan, t s well known that for n = 3, that s, n the case of the general cubc equaton x 3 + a x 2 + a 2 x + a 3 = 0, 2

5 a root x may be expressed as an rratonal functon of the three arbtrary coeffcents a, a 2, a 3, namely as the followng functon, whch s of the second order: x = b = f (a, a, a, a 2, a 3 ) = a 3 + a + c 2 a the radcal of hghest order, a, beng defned by the equaton a 3 = f (a, a, a 2, a 3 ) = c + a, and the subordnate radcal a beng defned by ths other equaton a 2 = f (a, a 2, a 3 ) = c 2 c 3 2, whle c and c 2 denote for abrdgment the followng two ratonal functons: c = 54 (2a3 9a a a 3 ), c 2 = 9 (a2 3a 2 ); so that, wth ths form of the rratonal functon b, the equaton b 3 + a b 2 + a 2 b + a 3 = 0 s satsfed, wthout any restrcton beng mposed on the three coeffcents a, a 2, a 3. For n = 4, that s, for the case of the general bquadratc equaton x 4 + a x 3 + a 2 x 2 + a 3 x + a 4 = 0, t s known n lke manner, that a root can be expressed as a fnte rratonal functon of the coeffcents, namely as the followng functon, whch s of the thrd order: x = b = f (a, a 2, a, a, a, a 2, a 3, a 4 ) = a 4 + a + a 2 + e 4 a ; a 2 ; wheren a 2 = f (a, a, a, a 2, a 3, a 4 ) = e 3 + a + e 2 a a 2 2 = f 2 (a, a, a, a 2, a 3, a 4 ) = e 3 + ρ 3 a + e 2 ρ 3 a a 3 = f (a, a, a 2, a 3, a 4 ) = e + a, a 2 = f (a, a 2, a 3, a 4 ) = e 2 e 3 2;,, 3

6 e 4, e 3, e 2, e denotng for abrdgment the followng ratonal functons: e 4 = 64 ( a3 + 4a a 2 8a 3 ), e 3 = 48 (3a2 8a 2 ), e 2 = 44 ( 3a a 3 + a a 4 ), e = 2 (3e 2e 3 e e 2 4) = 3456 (27a2 a 4 9a a 2 a 3 + 2a a 2 a a 2 3), and ρ 3 beng a root of the numercal equaton ρ ρ 3 + = 0. It s known also, that a root x of the same general bquadratc equaton may be expressed n another way, as an rratonal functon of the fourth order of the same arbtrary coeffcents a, a 2, a 3, a 4, namely the followng: x = b IV = f IV (a IV, a, a, a, a, a 2, a 3, a 4 ) = a 4 + a + a IV ; the radcal a IV beng defned by the equaton a IV2 = f (a, a, a, a, a 2, a 3, a 4 ) = a 2 + 3e 3 + 2e 4 whle a, a, a, and e 4, e 3, e 2, e, retan ther recent meanngs. Insomuch that ether the functon of thrd order b, or the functon of fourth order b IV, may be substtuted for x n the general bquadratc equaton; or, to express the same thng otherwse, the two equatons followng: b 4 + a b 3 + a 2 b 2 + a 3 b + a 4 = 0, and b IV4 + a b IV3 + a 2 b IV2 + a 3 b IV + a 4 = 0, are both dentcally true, n vrtue merely of the forms of the rratonal functons b and b IV, and ndependently of the values of the four arbtrary coeffcents a, a 2, a 3, a 4. But for hgher values of n the queston becomes more dffcult; and even for the case n = 5, that s, for the general equaton of the ffth degree, x 5 + a x 4 + a 2 x 3 + a 3 x 2 + a 4 x + a 5 = 0, the opnons of mathematcans appear to be not yet entrely agreed respectng the possblty or mpossblty of expressng a root as a functon of the coeffcents by any fnte combnaton of radcals and ratonal functons: or, n other words, respectng the possblty or mpossblty of satsfyng, by any rratonal functon b (m) of any fnte order, the equaton a b (m)5 + a b (m)4 + a 2 b (m)3 + a 3 b (m)2 + a 4 b (m) + a 5 = 0, 4,

7 the fve coeffcents a, a 2, a 3, a 4, a 5, remanng altogether arbtrary. To assst n decdng opnons upon ths mportant queston, by developng and llustratng (wth alteratons) the admrable argument of Abel aganst the possblty of any such expresson for a root of the general equaton of the ffth, or any hgher degree; and by applyng the prncples of the same argument, to show that no expresson of the same knd exsts for any root of any general but lower equaton, (quadratc, cubc, or bquadratc,) essentally dstnct from those whch have long been known; s the chef object of the present paper. [3.] In general, f we call an rratonal functon rreducble, when t s mpossble to express that functon, or any one of ts component radcals, by any smaller number of extractons of prme roots of varables, than the number whch the actual expresson of that functon or radcal nvolves; even by ntroducng roots of constant quanttes, or of numercal equatons, whch roots are n ths whole dscusson consdered as beng themselves constant quanttes, so that they nether nfluence the order of an rratonal functon, nor are ncluded among the radcals denoted by the symbols a, &c.; then t s not dffcult to prove that such rreducble rratonal functons possess several propertes n common, whch are adapted to assst n decdng the queston just now stated. In the frst place t may be observed, that, by an easy preparaton, the general rratonal functon b (m) of any order m may be put under the form b (m) = β (m) Σ <α (m) n whch the coeffcent b (m ) β (m),... β (m) n (m) exponent β (m) (m).(b (m ). a (m)β (m) β (m),... β (m)... a (m)β n (m) ), n (m) n (m) s a functon of the order m, or of a lower order; the s zero, or any postve nteger less than the prme number α (m), namely, as exponent nto the equaton of defnton of the radcal a (m) whch enters a (m)α(m) = f (m ) ; and the sgn of summaton extends to all the α (m).α (m) 2... α (m) β (m) terms whch have exponents n (m) subject to the condton just now mentoned. For, nasmuch as b (m) s, by supposton, a ratonal functon f (m) of all the radcals a (k) t s, wth respect to any radcal of hghest order, such as a (m), a functon of the form b (m) = n(a(m) ) m(a (m) ), m and n beng here used as sgns of some whole functons, or fnte ntegral polynomes. Now, f we denote by ρ α any root of the numercal equaton ρ (α ) α + ρ (α 2) α + ρ (α 3) α + + ρ 2 α + ρ α + = 0, 5,

8 so that ρ α s at the same tme a root of unty, because the last equaton gves ρ α α = ; and f we suppose the number α to be prme, so that ρ α, ρ 2 α, ρ 3 α,... ρ (α ) α are, n some arrangement or other, the α roots of the equaton above assgned: then, the product of all the α whole functons followng, m(ρ α a). m(ρ 2 αa)... m(ρ (α ) α a) = l(a), s not only tself a whole functon of a, but s one whch, when multpled by m(a), gves a product of the form l(a). m(a) = k(a α ), k beng here (as well as l) a sgn of some whole functon. If then we form the product m(ρ α (m) a (m) ). m(ρ 2 α (m) a (m) )... m(ρ α(m) α (m) a (m) ) = l(a (m) ), and multply, by t, both numerator and denomnator of the recently assgned expresson for b (m), we obtan ths new expresson for that general rratonal functon, b (m) = l(a(m) ). n(a (m) l(a (m) ) ). m(a (m) ) = l(a (m) ). n(a (m) k(a (m)α(m) ) ) = l(a(m) ). n(a (m) ) k(f (m ) ) = (a (m) ); the characterstc denotng here some functon, whch, relatvely to the radcal a (m), s whole, so that t may be thus developed, b (m) = (a (m) ) = 0 + a (m) + 2 a (m)2 + + r α (m)r, r beng a fnte postve nteger, and the coeffcents 0,,... r beng, n general, functons of the m th order, but not nvolvng the radcal a (m). And because the defnton of that radcal gves a (m)h = a (m)g. (f (m ) ) e, f h = g + eα (m), t s unnecessary to retan n evdence any of ts powers of whch the exponents are not less than α (m) ; we may therefore put the development of b (m) under the form b (m) = h 0 + h a (m) + + h α (m) 6 (a(m) ) α(m),

9 the coeffcents h 0, h,... beng stll, n general, functons of the m th order, not nvolvng the radcal a (m). It s clear that by a repetton of ths process of transformaton, the radcals a (m),... a (m) may all be removed from the denomnator of the ratonal functon f (m) ; and n (m) that ther exponents n the transformed numerator may all be depressed below the exponents whch defne those radcals: by whch means, the development above announced for the general rratonal functon b (m) may be obtaned; wheren the coeffcent b (m ) admts β (m),... β (m) n of beng analogously developed. (m) For example, the functon of the second order, b = a 3 + a + c 2 a whch was above assgned as an expresson for a root of the general cubc equaton, may be developed thus: n whch b = Σ.(b β <3 β b 0 = a 3, b =, b 2 = c 2 a 3. a β ) = b 0 + b a + b 2a 2 ;, = c 2 f = c 2 c + a. And ths last coeffcent b 2, whch s tself a functon of the frst order, may be developed thus: b 2 = c 2 c + a = b = Σ.(b β β. a β ) = b 0 + b a ; <2 n whch b 0 = c 2c c 2 = c 2c a 2 c 2 f Agan, the functon of the thrd order, = c 2c c 3 2 = c c 2 2 b = a 4 + a + a 2 + e 4 a, b = c 2. 2 a 2 whch expresses a root of the general bquadratc equaton, may be developed as follows:, n whch and b, = b = e 4 a 2. a 2 2 Σ.(b β <2 β 2 <2 β,β 2. a β. a β 2 2 ) = b 0,0 + b,0a + b 0,a 2 + b,a a 2 ; b 0,0 = a 4, b,0 =, b 0, =, = e 4 f. f 2 = ( = ( e 3 + ρ 2 e 3a + e ) 2 4 ρ 2. 3 a e 3 + a + e 2 a e 4 ) ( e 3 + ρ 3 a + e 2 ρ 3 a ) 7

10 And ths last coeffcent b,, whch s tself a functon of the second order, may be developed thus: b, = b = Σ.(b β <3 β. a β ) = b 0 + b a + b 2a 2 ; n whch b 0 = e 3, b = ρ2 3, b 2 = ρ 3e 2 ρ 3 e 2 e 4 e 4 e 4 a 3 = e 4 (e + a ) = ρ 3(e a ) e 4 e 2. 2 So that, upon the whole, these functons b and b, whch express, respectvely, roots of the general cubc and bquadratc equatons, may be put under the followng forms, whch nvolve no radcals n denomnators: and b = a ( ) a 3 + a + (c a 2 ), c 2 { b = a 4 + a + a 2 + ( ) } a e 3 + ρ 2 e 3a + ρ 3 (e a 2 ) a a 2 ; 4 e 2 and the functons f, f 2, whch enter nto the equatons of defnton of the radcals a, a 2, namely nto the equatons a 2 = f, a 2 2 = f 2, may n lke manner be expressed so as to nvolve no radcals n denomnators, namely thus: ( ) a a 2 = e 3 + a + (e a 2 ), ( ) a a 2 2 = e 3 + ρ 3 a + ρ 2 3(e a 2 ). e 2 It would be easy to gve other nstances of the same sort of transformaton, but t seems unnecessary to do so. [4.] It s mportant n the next place to observe, that any term of the foregong general development of the general rratonal functon b (m), may be solated from the rest, and expressed separately, as follows. Let b (m) denote a new rratonal functon, whch s γ (m),... γ (m) n (m) formed from b (m) by changng every radcal such as a (m) to a correspondng product such as ρ γ(m) α (m) a (m), n whch ρ (m) α b (m) γ (m),... γ (m) β (m) <α (m) n (m) = Σ e 2 s, as before, a root of unty; so that.(b (m ) β (m),... β (m) n (m). ρ β (m) γ (m) α (m)... ρ β(m) γ(m) n (m) n (m) α (m) n (m). a (m)β (m) and let any solated term of the correspondng development of b (m) or b (m) 0,... 0 the symbol t (m) β (m),... β (m) n (m) = b (m ). a (m)β (m) β (m),... β (m)... a (m)β n (m) 8 (m)... a (m)β n (m) ); n (m) (m) n (m) n (m) ; be denoted by

11 we shall then have, as the announced expresson for the solated term, the followng: t (m) β (m),... β (m) n (m) =. α (m)... α (m) Σ n (m) γ (m) <α (m).(b (m) γ (m),... γ (m) α (m). ρ β n (m) (m) γ (m)... ρ β(m) γ(m) n (m) n (m) ); α (m) n (m) the sgn of summaton here extendng to all those terms n whch every ndex such as γ (m) s equal to zero or to some postve nteger less than α (m). Thus, n the case of the functon of second order b, whch represents, as we have seen, a root of the general cubc equaton, f we wsh to obtan an solated expresson for any term of ts development already found, namely the development t β b = Σ.(b β <3 β we have only to ntroduce the functon b γ = Σ.(b β <3 β and to employ the formula t β In partcular, n whch = b β. a β = 3. Σ.(b γ <3 and n whch t s to be remembered that. a β ) = b 0 + b a + b 2a 2 = t 0 + t + t 2,. ρ β γ 3. a β ) = b 0 + b ρ γ γ 3 a + b 2ρ 2γ 3 b 3 a 2,. ρ β γ 3 ) = 3 (b 0 + ρ β + ρ 2β 2). t 0 = b 0 = 3 (b 0 + b + b 2), t = b a = 3 (b 0 + ρ 3 b + ρ 2 3 b 2), t 2 = b 2a 2 = 3 (b 0 + ρ 2 3 b + ρ 4 3 b 2), b 0 = b 0 + b a + b 2a 2 (= b ), b = b 0 + b ρ 3 a + b 2ρ 2 3a 2, b 2 = b 0 + b ρ 2 3a + b 2ρ 4 3a 2, ρ ρ 3 + = 0, and therefore ρ 3 3 =. 3 b Agan, f we wsh to solate any term t β of the development above assgned for the,β 2 functon of thrd order b, whch represents a root of the general bquadratc equaton, we may employ the formula t β,β 2 = b β,β 2. a β. a β 2 2 = 2.2. Σ γ <2 γ 2 <2.(b γ,γ 2. ρ β γ 2. ρ β = 4 {b 0,0 + ( ) β b,0 + ( ) β 2 b 0, + ( ) (β +β 2 ) b,}; 9 2 γ 2 2 )

12 n whch we have ntroduced the functon b γ,γ 2 = Σ.(b β <2 β 2 <2 β,β 2. ρ β γ 2. ρ β 2 γ 2 2. a β. a β 2 2 ) = b 0,0 + ( ) γ b,0a + ( ) γ 2 b 0,a 2 + ( ) γ +γ 2 b,a a 2 ; so that, n partcular, we have the four expressons n whch t 0,0 = b 0,0 = 4 (b 0,0 + b,0 + b 0, + b,), t,0 = b,0a = 4 (b 0,0 b,0 + b 0, b,), t 0, = b 0,a 2 = 4 (b 0,0 + b,0 b 0, b,), t, = b,a a 2 = 4 (b 0,0 b,0 b 0, + b,), b 0,0 = b 0,0 + b,0a + b 0,a 2 + b,a a 2, b,0 = b 0,0 b,0a + b 0,a 2 b,a a 2, b 0, = b 0,0 + b,0a b 0,a 2 b,a a 2, b, = b 0,0 b,0a b 0,a 2 + b,a a 2. In these examples, the truth of the results s obvous; and the general demonstraton follows easly from the propertes of the roots of unty. [5.] We have htherto made no use of the assumed rreducblty of the rratonal functon b (m). But takng now ths property nto account, we soon perceve that the component radcals a (k), whch enter nto the composton of ths rreducble functon, must not be subject to, nor even compatble wth, any equatons or equaton of condton whatever, except only the equatons of defnton, whch determne those radcals a (k), by determnng ther prme powers a (k)α(k). For the exstence or possblty of any such equaton of condton n conjuncton wth those equatons of defnton, would enable us to express at least one of the above mentoned radcals as a ratonal functon of others of the same system, and of orders not hgher than ts own, or even, perhaps, as a ratonal functon of the orgnal varables a,... a n, though multpled n general by a root of a numercal equaton; and therefore would enable us to dmnsh the number of extractons of prme roots of functons, whch would be nconsstent wth the rreducblty supposed. If fact, f any such equaton of condton, nvolvng any radcal or radcals of order k, but none of any hgher order, were compatble wth the equatons of defnton; then, by some obvous preparatons, such as brngng the equaton of condton to the form of zero equated to some fnte polynomal functon of some radcal a (k) of the k th order; and rejectng, by the methods of equal roots and of the greatest common measure, all factors of ths polynome, except those whch are unequal among themselves, and are ncluded among the factors of that other polynome whch s equated to zero n the correspondng form of the equaton of defnton of the radcal a (k) ; we should fnd that ths last equaton of defnton a (k)α(k) f (k ) = 0 0

13 must be dvsble, ether dentcally, or at least for some sutable system of values of the remanng radcals, by an equaton of condton of the form a (k)g + g (k) a(k)g + + g (k) g a(k) + g (k) g = 0; g beng less than α (k), and the coeffcents g (k),... g(k) g beng functons of orders not hgher than k, and not nvolvng the radcal a (k). Now, f we were to suppose that, for any system of values of the remanng radcals, the coeffcents g (k),... should all be = 0, or ndeed f even the last of those coeffcents should thus vansh, we should then have a new equaton of condton, namely the followng: f (k ) = 0, whch would be oblged to be compatble wth the equatons of defnton of the remanng radcals, and would therefore ether conduct at last, by a repetton of the same analyss, to a radcal essentally vanshng, and consequently superfluous, among those whch have been supposed to enter nto the composton of the functon b (m) ; or else would brng us back to the dvsblty of an equaton of defnton by an equaton of condton, of the form just now assgned, and wth coeffcents g (k),... g(k) g whch would not all be = 0. But for ths purpose t would be necessary that a relaton, or system of relatons, should exst (or at least should be compatble wth the remanng equatons of defnton,) of the form g (k) g e = ν e a (k)e, e beng less than α (k), and ν e beng dfferent from zero, and beng a root of a numercal equaton; and because α (k) s prme, we could fnd nteger numbers λ and µ, whch would satsfy the condton λα (k) µe = ; so that, fnally, we should have an expresson for the radcal a (k), as a ratonal functon of others of the same system, and of orders not hgher than ts own, though multpled n general (as was above announced) by a root of a numercal equaton; namely the followng expresson: a (k) = ν e µ g (k) µ g e f (k )λ. And f we should suppose ths last equaton to be not dentcally true, but only to hold good for some systems of values of the remanng radcals, of orders not hgher than k, we should stll obtan, at least, an equaton of condton between those remanng radcals, by rasng the expresson just found for a (k) to the power α (k) f (k ) (ν µ e g (k) µ g e ; namely the followng equaton of condton, f (k )λ ) α(k) = 0, whch mght then be treated lke the former, tll at last an expresson should be obtaned, of the knd above announced, for at least one of the remanng radcals. In every case, therefore,

14 we should be conducted to a dmnuton of the number of prme roots of varables n the expresson of the functon b (m), whch consequently would not be rreducble. For example, f an rratonal functon of the m th order contan any radcal a (m) of the cubc form, ts exponent α (m) of defnton beng of the form of the cubc form, ts exponent α (m) α (m)3 = f (m ) (a (m ),... a (m ),... a n (m ),... a n ); beng = 3, and ts equaton f also the other equatons of defnton permt us to suppose that ths radcal may be equal to some ratonal functon of the rest, so that an equaton of the form a (m) + g (m) = 0, (n whch the functon g (m) does not contan the radcal a (m),) s compatble wth the equaton of defnton a (m)3 f (m ) = 0; then, from the forms of these two last mentoned equatons, the latter must be dvsble by the former, at least for some sutable system of values of the remanng radcals: and therefore the followng relaton, whch does not nvolve the radcal a (m), namely, f (m ) + g (m)3 = 0, must be ether dentcally true, n whch case we may substtute for the radcal a (m), n the proposed functon of the m th order, the expresson a (m) = 3. g (m) ; or at least t must be true as an equaton of condton between the remanng radcals, and lable as such to a smlar treatment, conductng to an analogous result. A more smple and specfc example s suppled by the followng functon of the second order, x = a ( ) ( ) c + c 2 c c c 2 c3 2, whch s not uncommonly proposed as an expresson for a root x of the general cubc equaton x 3 + a x 2 + a 2 x + a 3 = 0, c and c 2 beng certan ratonal functons of a, a 2, a 3, whch were assgned n a former artcle, and whch are such that the cubc equaton may be thus wrtten: ( x + a 3 ) 3 3c2 ( x + a 3 2 ) 2c = 0.

15 Puttng ths functon of the second order under the form n whch the radcals are defned as follows, x = a 3 + a + a 2, a 3 = c + a, a 3 2 = c a, a 2 = c 2 c 3 2, we easly perceve that t s permtted by these defntons to suppose that the radcals a, a 2 are connected so as to satsfy the followng equaton of condton, a a 2 = c 2 ; and even that ths supposton must be made, n order to render the proposed functon of the second order a root of the cubc equaton. But the mere knowledge of the compatblty of the equaton of condton a 2 c 2 a = 0 wth the equaton of defnton a 3 2 (c a ) = 0, s suffcent to enable us to nfer, from the forms of these two equatons, that the latter s dvsble by the former, at least for some sutable system of values of the remanng radcals a and a, consstent wth ther equatons of defnton; and therefore that the followng relaton and the expresson c a ( ) 3 c2 a = 0, a 2 = 3. c 2 are at least consstent wth those equatons. In the present example, the relaton thus arrved at s found to be dentcally true, and consequently the radcals a and a reman ndependent of each other; but for the same reason, the radcal a 2 may be changed to the expresson just now gven; so that the proposed functon of the second order, a x = a 3 + a + a 2, may, by the mere defntons of ts radcals, and even wthout attendng to the cubc equaton whch t was desgned to satsfy, be put under the form x = a 3 + a + 3. c 2 a the number of prme roots of varables beng depressed from three to two; and consequently that proposed functon was not rreducble n the sense whch has been already explaned. 3,,

16 [6.] From the foregong propertes of rratonal and rreducble functons, t follows easly that f any one value of any such functon b (m), correspondng to any one system of values of the radcals on whch t depends, be equal to any one root of any equaton of the form x s + a x s + + a s x + a s = 0, n whch the coeffcents a,... a s are any ratonal functons of the n orgnal quanttes a,... a n ; n such a manner that for some one system of values of the radcals a, &c., the equaton b (m)s + a b (m)s + + a s = 0 s satsfed: then the same equaton must be satsfed, also, for all systems of values of those radcals, consstent wth ther equatons of defnton. It s an mmedate consequence of ths result, that all the values of the functon whch has already been denoted by the symbol b (m) must represent roots of the same equaton of the s th degree; and the γ (m),... γ (m) n (m) same prncples show that all these values of b (m) must be unequal among themselves, and γ (m) therefore must represent so many dfferent roots x, x 2,... of the same equatons x s +&c. = 0, f every ndex or exponent γ (m) be restrcted, as before, to denote ether zero or some postve nteger number less than the correspondng exponent α (m) : for f, wth ths restrcton, any two of the values of b (m) could be supposed equal, an equaton of condton between the γ (m),... radcals a (m), &c. would arse, whch would be nconsstent wth the supposed rreducblty of the functon b (m). For example, havng found that the cubc equaton... x 3 + a x 2 + a 2 x + a 3 = 0 s satsfed by the rratonal and rreducble functon b above assgned, we can nfer that the same equaton s satsfed by all the three values b 0, b, b 2 of the functon b γ ; and that these three values must be all unequal among themselves, so that they must represent some three unequal roots x, x 2, x 3, and consequently all the three roots of the cubc equaton proposed. [7.] Combnng the result of the last artcle wth that whch was before obtaned respectng the solatng of a term of a development, we see that f any root x of any proposed equaton, of any degree s, n whch the s coeffcents a,... a s are stll supposed to be ratonal functons of the n orgnal quanttes a,... a n, can be expressed as an rratonal and rreducble functon b (m) of those orgnal quanttes; and f that functon b (m) be developed under the form above assgned; then every term t (m) β (m),... of ths development may be expressed as a ratonal (and ndeed lnear) functon of some or all of the s roots x, x 2,... x s of the same proposed equaton. For example, when we have found that a root x of the cubc equaton x 3 + a x 2 + a 2 x + a 3 = 0 4

17 can be represented by the rratonal and rreducble functon already mentoned, x = b = b 0 + b a + b 2a 2 = t 0 + t + t 2, (n whch b =,) we can express the separate terms of ths last development as follows, t 0 = b 0 = 3 (x + x 2 + x 3 ), t = b a = 3 (x + ρ 3 x 2 + ρ 2 3 x 3), t 2 = b 2a 2 = 3 (x + ρ 2 3 x 2 + ρ 4 3 x 3); namely, by changng b 0, b, b 2 to x, x 2, x 3 n the expressons found before for t 0, t, t 2. In lke manner, when a root x of the bquadratc equaton s represented by the rratonal functon x 4 + a x 3 + a 2 x 2 + a 3 x + a 4 = 0 x = b = b 0,0 + b,0a + b 0,a 2 + b,a a 2 = t 0,0 + t,0 + t 0, + t,, n whch b,0 = b 0, =, we easly derve, from results obtaned before, (by merely changng b 0,0, b 0,, b,0, b, to x, x 2, x 3, x 4,) the followng expressons for the four separate terms of ths development: t 0,0 = b 0,0 = 4 (x + x 2 + x 3 + x 4 ), t,0 = b,0a = 4 (x + x 2 x 3 x 4 ), t 0, = b 0,a 2 = 4 (x x 2 + x 3 x 4 ), t, = b,a a 2 = 4 (x x 2 x 3 + x 4 ); x, x 2, x 3, x 4 beng some four unequal roots, and therefore all the four roots of the proposed bquadratc equaton. And when that equaton has a root represented n ths other way, whch also has been already ndcated, and n whch b =, x = b IV = a 4 + a + a IV = b 0 + b a IV = t IV 0 + t IV, then each of the two terms of ths development may be separately expressed as follows, t IV 0 = b = 2 (x + x 2 ), t IV = b a IV = 2 (x x 2 ), x and x 2 beng some two unequal roots of the same bquadratc equaton. A stll more smple example s suppled by the quadratc equaton, x 2 + a x + a 2 = 0; 5

18 for when we represent a root x of ths equaton as follows, x = b = a 2 + a = t 0 + t, we have the followng well-known expressons for the two terms t 0, t, as ratonal and lnear functons of the roots x, x 2, t 0 = a = 2 2 (x + x 2 ), t = a = 2 (x x 2 ). In these examples, the radcals of hghest order, namely a n b, a n b, a and a 2 n b, and a IV n b IV, have all had the coeffcents of ther frst powers equal to unty; and consequently have been themselves expressed as ratonal (though unsymmetrc) functons of the roots of that equaton n x, whch the functon b (m) satsfes; namely, a = 2 (x x 2 ), a = 3 (x + ρ 2 3x 2 + ρ 3 x 3 ), a = 4 (x + x 2 x 3 x 4 ), a 2 = 4 (x x 2 + x 3 x 4 ), a IV = 2 (x x 2 ); the frst expresson beng connected wth the general quadratc, the second wth the general cubc, and the three last wth the general bquadratc equaton. We shall soon see that all these results are ncluded n one more general. [8.] To llustrate, by a prelmnary example, the reasonngs to whch we are next to proceed, let t be supposed that any two of the terms t (m) are of the forms β (m),... and t 2,,3,4 = b 2,,3,4a 2 a 2a 3 3 a 4 4, t,,2,3 = b,,2,3a a 2a 2 3 a 3 4, n whch the radcals are defned by equatons such as the followng a 3 = f, a 3 2 = f 2, a 5 3 = f 3, a 5 4 = f 4, ther exponents α, α 2, α 3, α 4 beng respectvely equal to the numbers 3, 3, 5, 5. We shall then have, by rasng the two terms t to sutable powers, and attendng to the equatons of defnton, the followng expressons: t 0 2,,3,4 = b 0 2,,3,4f 6 f 2 3 f 3 6 f 4 8 a 2 a 2; t 0,,2,3 = b 0,,2,3f 3 f 2 3 f 3 4 f 4 6 a a 2; t 6 2,,3,4 = b 6 2,,3,4f 4 f 2 2 f 3 3 f 4 4 a 3 3 a 4 4 ; t 6,,2,3 = b 6,,2,3f 2 f 2 2 f 2 3 f 3 4 a 2 3 a 3 4 ; 6

19 whch gve f we put, for abrdgment, t = c a, t 2 = c 2a 2, t 3 = c 3a 3, t 4 = c 4a 4, t = t 0 2,,3,4t 0,,2,3 ; t 2 = t 0 2,,3,4 t 20,,2,3; t 3 = t 8 2,,3,4t 24,,2,3 ; t 4 = t 2 2,,3,4 t 8,,2,3; c = b 0 2,,3,4b 0,,2,3 f 3 f 2 3 f 2 4 ; c 2 = b 0 2,,3,4 b 20,,2,3f 2 3 f 3 2 f 4 4 ; c 3 = b 8 2,,3,4b 24,,2,3 f 4 f 2 2 f 3; c 4 = b 2 2,,3,4 b 8,,2,3f 2 f 2 2 f 4. And, wth a lttle attenton, t becomes clear that the same sort of process may be appled to the terms t (m) of the development of any rreducble functon β (m),... b(m) ; so that we have, n general, a system of relatons, such as the followng: n whch t (m) of the varous terms t (m) β (m) t (m) = c (m ) a (m) ;... t (m) n (m),... = c (m ) a (m) ; n (m) n (m) s the product of certan powers (wth exponents postve, or negatve, or null) ; and the coeffcent c(m ) s dfferent from zero, but s of an order lower than m. For f any radcal of the order m were supposed to be so nextrcably connected, n every term, wth one or more of the remanng radcals of the same hghest order, that t could not be dsentangled from them by a process of the foregong knd; and that thus the foregong analyss of the functon b (m) should be unable to conduct to separate expressons for those radcals; t would then, recprocally, have been unnecessary to calculate them separately, n effectng the synthess of that functon; whch functon, consequently, would not be rreducble. If, for example, the exponents α (m) and α (m) 2, whch enter nto the equatons of defnton of the radcals a (m) and a (m) 2 should both be = 3, so that those radcals should both be cube-roots of functons of lower orders; and f these two cube-roots should enter only by ther product, so that no analyss of the foregong knd could obtan them otherwse than n connexon, and under the form c (m ) a (m) a (m) 2 ; t would then have been suffcent, n effectng the synthess of b (m), to have calculated only the cube-root of the product a (m)3 a (m)3 2 = f (m ) f (m ) 2 = f (m ), nstead of calculatng separately the cuberoots of ts two factors a (m)3 = f (m ), and a (m)3 2 = f (m ) 2 : the number of extractons of prme roots of varables mght, therefore, have been dmnshed n the calculaton of the functon b (m), whch would be nconsstent wth the rreducblty of that functon. In the cases of the rreducble functons b, b, b, b IV, whch have been above assgned, as representng roots of the general quadratc, cubc, and bquadratc equatons, the theorem of the present artcle s seen at once to hold good; because n these the radcals of hghest order are themselves terms of the developments n queston, the coeffcents of ther frst powers beng already equal to unty. Thus n the development of b, we have a = t ; n b, we have a = t ; n b, we have a = t,0, and a 2 = t 0,; and n b IV, we have a IV = t IV [9.] By rasng to the proper powers the general expressons of the form t (m) = c (m ) a (m), 7.

20 we obtan a system of n (m) equatons of ths other form t (m)α(m) = c (m )α(m) f (m ) = f (m ), beng some new rratonal functon, of an order lower than m; and by combnng the same expressons wth those whch defne the varous terms t (m), the number of whch β (m),... f (m ) terms we shall denote by the symbol t (m), we obtan another system of t (m) equatons, of whch the followng s a type, f we put, for abrdgment, u (m ) β (m),... β (m) n (m) = b (m ) β (m),... β (m) n (m), and u (m ) β (m) b (m ) β (m) β (m),... = t(m) =,... b(m ) β (m). (m),... t(m) β. (m),... c(m ) β t (m) β (m) n (m) n (m), c (m ) β (m) n (m) n (m). In ths manner we obtan n general n (m) + t (m) equatons, n each of whch the product of certan powers, (wth postve, negatve, or null exponents,) of the t (m) terms of the development of the rratonal functon b (m), s equated to some other rratonal functon, f (m ) or b (m ), of an order lower than m. Indeed, t s to be observed, that snce these varous equatons are obtaned by an elmnaton of the n (m) radcals of hghest order, between ther n (m) equatons of defnton and the t (m) expressons for the t (m) terms of the development of b (m), they cannot be equvalent to more than t (m) dstnct relatons. But, among them, they must nvolve explctly all the radcals of lower orders, whch enter nto the composton of the rreducble functon b (m). For f any radcal a (k), of order lower than m, were wantng n all the n (m) + t (m) functons of the forms f (m ) and b (m ) β (m),..., we mght then employ nstead of the old system of radcals a (m),... of the order m, a new and equally numerous system of radcals a (m),... accordng to the followng type, a (m) = t (m) = α(m) f (m ) ; and mght then express all the t (m) terms of b (m), by means of these new radcals, accordng to the formula... a (m)β (m) n (m) t (m) β (m) =,... b (m ) β (m). (m),... a (m)β 8 n (m),

21 whch would not nvolve the radcal a (k) ; so that n ths way the number of extractons of prme roots of varables mght be dmnshed, whch would be nconsstent wth the rreducblty of b (m). The results of the present artcle may be exemplfed n the case of any one of the functons b, b, b, b IV, whch have already been consdered. Thus, n the case of the functon b, whch represents a root of the general cubc equaton, we have t = t, c =, f = f, β β = b β, u β and the n (m) + t (m) = + 3 = 4 followng relatons hold good: = t β t 3 = f, t 0 = b 0, = b, t 2t 2 = b 2;. t β, of whch ndeed the thrd s dentcally true, and the second does not nvolve a, because b 0 = a 3 ; but both the frst and fourth of these relatons nvolve that radcal a, because f = c + a, and b 2 = c a c 2. 2 [0.] Snce each of the t (m) terms of the development of b (n) can be expressed as a ratonal functon of the s roots x,... x s of that equaton of the s th degree whch b (m) s supposed to satsfy; t follows that every ratonal functon of these t (m) terms must be lkewse a ratonal functon of those s roots, and must admt, as such, of some fnte number r of values, correspondng to all possble changes of arrangement of the same s roots amongst themselves. The same term or functon must, for the same reason, be tself a root of an equaton of the r th degree, of whch the coeffcents are symmetrcal functons of the s roots, x,... x s, and therefore are ratonal functons of the s coeffcents a,... a s, and ultmately of the n orgnal quanttes a,... a n ; whle the r other roots of ths new equaton are the r other values of the same functon of x,... x s, correspondng to the changes of arrangement just now mentoned. Hence, every one of the n (m) + t (m) functons t (m)α(m) u (m ), and therefore also every one of the β (m),... n(m) + t (m) functons f (m ) and and b (m ), to β (m),... whch they are respectvely equal, and whch have been shown to contan, among them, all the radcals of orders lower than m, must be a root of some such new equaton, although the degree r wll not n general be the same for all. Treatng these new equatons and functons, and the radcals of the order m, as the equaton x s + &c. = 0, the functon b (m), and the radcals of the order m have already been treated; we obtan a new system of relatons, analogous to those already found, and capable of beng thus denoted: t (m ) t (m )α(m ) u (m ) β (m ) = c (m 2) a (m ) ; = f (m 2) ; =,... b (m 2). β (m ),... And so proceedng, we come at last to a system of the form, t = c a,... t n = c n a n ; 9

22 n whch the coeffcent c s dfferent from zero, and s a ratonal functon of the n orgnal quanttes a,... a n ; whle t s a ratonal functon of the s roots x,... x s of that equaton of the s th degree n x whch t has been suppose that b (m) satsfes. We have therefore the expresson a = t c ; whch enables us to consder every radcal a of the frst order, as a ratonal functon f of the s roots x,... x s, and of the n orgnal quanttes a,... a n : so that we may wrte a = f (x,... x s, a,... a n ). But before arrvng at the last mentoned system of relatons, another system of the form t = c a,... t n = c n a n must have been found, n whch the coeffcent c s dfferent from zero, and s a ratonal functon of a,... a n and of a,..., a n, whle t s a ratonal functon of x,... x s ; we have therefore the expresson a = t c and we see that every radcal of the second order also s equal to a ratonal functon of x,... x s and of a,... a n : so that we may wrte a = f (x,... x s, a,... a n ). And re-ascendng thus, through orders hgher and hgher, we fnd, fnally, by smlar reasonngs, that every one of the n + n + + +n (k) + + n (m) radcals whch enter nto the composton of the rratonal and rreducble functon b (m), such as the radcal a (k), must be expressble as a ratonal functon f (k) of the roots x,... x s, and of the orgnal quanttes a,... a n : so that we have a complete system of expressons, for all these radcals, whch are ncluded n the general formula a (k) = f (k) (x,... x s, a,... a n ). Thus, n the case of the cubc equaton and the functon b, when we have arrved at the relaton t 3 = f, n whch we fnd that the ratonal functon t = 3 (x + ρ 2 3x 2 + ρ 3 x 3 ), and f = c + a, t 3 = 27 (x + ρ 2 3x 2 + ρ 3 x 3 ) 3 20,

23 admts only of two dfferent values, n whatever way the arrangement of the three roots x, x 2, x 3 may be changed; t must therefore be tself a root of a quadratc equaton, n whch the coeffcents are symmetrc functons of those three roots, and consequently ratonal functons of a, a 2, a 3 ; namely, the equaton 0 = (t 3 ) 2 27 {(x + ρ 2 3x 2 + ρ 3 x 3 ) 3 + (x + ρ 2 3x 3 + ρ 3 x 2 ) 3 }(t 3 ) (x + ρ 2 3x 2 + ρ 3 x 3 ) 3 (x + ρ 2 3x 3 + ρ 3 x 2 ) 3 ( ) a = (t 3 ) (2a3 9a a a 3 )(t ) + 3a 2. 9 The same quadratc equaton must therefore be satsfed when we substtute for t 3 the functon x + a to whch t s equal, and n whch a s a square root; t must therefore be satsfed by both values of the functon c ± a, because the radcal a must be subject to no condton except that by whch ts square s determned; therefore, ths radcal a must be equal to the sem-dfference of two unequal roots of the same quadratc equaton; that s, to the sem-dfference of the two values of the ratonal functon t 3 ; whch sem-dfference s tself a ratonal functon of x, x 2, x 3, namely a = 54 {(x + ρ 2 3x 2 + ρ 3 x 3 ) 3 (x + ρ 2 3x 3 + ρ 3 x 2 ) 3 } = 8 (ρ2 3 ρ 3 )(x x 2 )(x x 3 )(x 2 x 3 ) = f (x, x 2, x 3 ). The same concluson would have been obtaned, though n a somewhat less smple way, f we had employed the relaton t 2t 2 = b 2, n whch t 2t 2 = 3(x + ρ 2 3x 3 + ρ 3 x 2 ) (x + ρ 2 3 x 2 + ρ 3 x 3 ) 2, b 2 = c a [.] In general, let p be the number of values whch the ratonal functon f (k) can receve, by alterng n all possble ways the arrangements of the s roots x,... x s, these roots beng stll treated as arbtrary and ndependent quanttes, (so that p s equal ether to the product s, or to some submultple of that product); we shall then have an dentcal equaton of the form f (k)p + d f (k)p c d p f (k) + d p = 0, n whch the coeffcents d,... d p are ratonal functons of a,... a n ; and therefore at least one value of the radcal a (k) must satsfy the equaton a (k)p + d a (k)p + + d p a (k) + d p = 0. But n order to do ths, t s necessary, for reasons already explaned, that all values of the same radcal a (k), obtaned by multplyng tself and all ts subordnate radcals of the same 2.

24 functonal system by any powers of the correspondng roots of unty, should satsfy the same equaton; and therefore that the number q of these values of the radcal a (k) should not exceed the degree p of that equaton, or the number of the values of the ratonal functon f (k). Agan, snce we have denoted by q the number of values of the radcal, we must suppose that t satsfes dentcally an equaton of the form a (k)q + e a (k)q + + e q a (k) + e q = 0, the coeffcents e,... e q beng ratonal functons of a,... a n ; and therefore that at least one value of the functon f (k) satsfes the equaton f (k)q + e. f (k)q + + e q f (k) = 0. Suppose now that the s roots x,... x s of the orgnal equaton n x, x s + a x s + + a s x + a s = 0, are really unconnected by any relaton among themselves, a supposton whch requres that s should not be greater than n, snce a,... a s are ratonal functons of a,... a n ; suppose also that a,... a n can be expressed, recprocally, as ratonal functons of a,... a s, a supposton whch requres, recprocally, that n should not be greater than s, because the orgnal quanttes a,... a n are, n ths whole dscusson, consdered as ndependent of each other. Wth these suppostons, whch nvolve the equalty s = n, we may consder the n quanttes a,... a n, and therefore also the q coeffcents e,... e q, as beng symmetrc functons of the n roots x,... x n of the equaton we may also consder f (k) roots, so that we may wrte and snce the truth of the equaton x n + a x n + + a n x + a n = 0; as beng a ratonal but unsymmetrc functon of the same n arbtrary a k = f (k) (x,... x n ); f (k)q + e f (k)q + + e q = 0 must depend only on the forms of the functons, and not on the values of the quanttes whch t nvolves, (those values beng altogether arbtrary,) we may alter n any manner the arrangement of those n arbtrary quanttes x,... x n, and the equaton must stll hold good. But by such changes of arrangement, the symmetrc coeffcents e,... e q reman unchanged, whle the ratonal but unsymmetrc functon f (k) takes, n successon, all those p values of whch t was before supposed to be capable; thse p unequal values therefore must all be roots of the same equaton of the q th degree, and consequently q must not be less than p. And snce t has been shown that the former of these two last mentoned numbers must not exceed the latter, t follows that they must be equal to each other, so that we have the relaton q = p : 22

25 that s, the radcal a (k) and the ratonal functon f (k) must be exactly coextensve n multplcty of value. For example, when, n consderng the rreducble rratonal expresson b for a root of the general cubc, we are conducted to the relaton assgned n the last artcle, a = f (x, x 2, x 3 ) = 8 (ρ3 3 ρ 3 )(x x 2 )(x x 3 )(x 2 x 3 ); we can then at pleasure nfer, ether that the radcal a must admt (as a radcal) of two and only two values, f we have prevously perceved that the ratonal functon f admts (as a ratonal functon) of two values, and only two, correspondng to changes of arrangement of the three roots x, x 2, x 3, namely, the two followng values, whch dffer by ther sgns, ± 8 (ρ3 3 ρ 3 )(x x 2 )(x x 3 )(x 2 x 3 ); or else we may nfer that the functon f admts thus of two values and two only, for all changes of arrangement of x, x 2, x 3, f we have perceved that the radcal a (as beng gven by ts square, a 2 = f = c 2 c 3 2, whch square s ratonal,) admts, tself, of the two values ±a whch dffer n ther sgns. [2.] The condtons assumed n the last artcle are all fulflled, when we suppose the coeffcents a &c. to concde wth the n orgnal quanttes a, &c., that s, when we return to the equaton orgnally proposed; x n + a x n + + a n x + a n = 0, whch s the general equaton of the n th degree: so that we have, for any radcal a (k), whch enters nto the composton of any rratonal and rreducble functon representng any root of any such equaton, an expresson of the form a (k) = f (k) (x,... x n ); the radcal and the ratonal functon beng coextensve n multplcty of value. We are, therefore, conducted thus to the followng mportant theorem, to whch Abel frst was led, by reasonngs somewhat dfferent from the foregong: namely, that f a root x of the general equaton of any partcular degree n can be expressed as an rreducble rratonal functon b (m) of the n arbtrary coeffcents of that equaton, then every radcal a (k), whch enters nto the composton of that functon b (m), must admt of beng expressed as a ratonal, though unsymmetrc functon f (k) of the n arbtrary roots of the same general equaton; and ths ratonal but unsymmetrc functon f (k) must admt of recevng exactly the same varety of values, through changes of arrangement of the n roots on whch t depends, as that whch the radcal a (k) can receve, through multplcatons of tself and of all ts subordnate functonal radcals by any powers of the correspondng roots of unty. Examples of the truth of ths theorem have already been gven, by antcpaton, n the seventh and tenth artcles of ths Essay; to whch we may add, that the radcals a and a, 23

26 n the expressons gven above for a root of the general bquadratc, admt of beng thus expressed: a = 48 {(x + x 2 x 3 x 4 ) 2 + ρ 2 3(x x 2 + x 3 x 4 ) 2 + ρ 3 (x x 2 x 3 + x 4 ) 2 } = 2 {x x 2 + x 3 x 4 + ρ 2 3(x x 3 + x 2 x 4 ) + ρ 3 (x x 4 + x 2 x 3 )}; a = 3456 {x x 2 + x 3 x 4 + ρ 2 3(x x 3 + x 2 x 4 ) + ρ 3 (x x 4 + x 2 x 3 )} {x x 2 + x 3 x 4 + ρ 2 3(x x 4 + x 2 x 3 ) + ρ 3 (x x 3 + x 2 x 4 )} 3 = 52 (ρ2 3 ρ 3 )(x x 2 )(x x 3 )(x x 4 )(x 2 x 3 )(x 2 x 4 )(x 3 x 4 ). But before we proceed to apply ths theorem to prove, n a manner smlar to that of Abel, the mpossblty of obtanng any fnte expresson, rratonal and rreducble, for a root of the general equaton of the ffth degree, t wll be nstructve to apply t, n a new way, (accordng to the announcement made n the second artcle,) to equatons of lower degrees; so as to draw, from those lower equatons, a class of llustratons qute dfferent from those whch have been heretofore adduced: namely, by showng, à pror, wth the help of the same general theorem, that no new fnte functon, rratonal and rreducble, can be found, essentally dstnct n ts radcals from those whch have long snce been dscovered, for expressng any root of any such lower but general equaton, quadratc, cubc or bquadratc, n terms of the coeffcents of that equaton. [3.] Begnnng then wth the general quadratc, x 2 + a x + a 2 = 0, let us endeavour to nvestgate, à pror, wth the help of the foregong theorem, all possble forms of rratonal and rreducble functons b (m), whch can express a root x of ths quadratc, n terms of the two arbtrary coeffcents a, a 2, so as to satsfy dentcally, or ndependently of the values of those two coeffcents, the equaton b (m)2 + a b (m) + a 2 = 0. The two roots of the proposed quadratc beng denoted by the symbols x and x 2, we know that the two coeffcents a and a 2 are equal to the followng symmetrc functons, a = (x + x 2 ), a 2 = x x 2 ; we cannot therefore suppose ether root to be a ratonal functon b of these coeffcents, because an unsymmetrc functon of two arbtrary quanttes cannot be equal to a symmetrc functon of the same; and consequently we must suppose that the exponent m of the order of the sought functon b (m) s greater than 0. The expresson b (m) for x must therefore nvolve at least one radcal a, whch must tself admt of beng expressed as a ratonal but unsymmetrc functon of the two roots x, x 2, a = f (x, x 2 ), 24

27 and of whch some prme power can be expressed as a ratonal functon of the two coeffcents a, a 2, a α = f(a, a 2 ), the exponent α beng equal to the number of the values f (x, x 2 ), f (x 2, x ), of the unsymmetrc functon f, and consequently beng = 2; so that the radcal a must be a square root, and must have two values dfferng n sgn, whch may be thus expressed: +a = f (x, x 2 ), a = f (x 2, x ). But, n general, whatever ratonal functon may be denoted by f, the quotents f(x, x 2 ) + f(x 2, x ) 2 and f(x, x 2 ) f(x 2, x ) 2(x x 2 ) are some symmetrc functons, a and b; so that we may put generally therefore, snce we have, at present, the functon f must be of the form f(x, x 2 ) = a + b(x x 2 ), f(x 2, x ) = a b(x x 2 ); f (x 2, x ) = f (x, x 2 ), f (x, x 2 ) = b(x x 2 ), the multpler b beng symmetrc. At the same tme, and therefore the functon f s of the form so that the radcal a may be thus expressed, a = b(x x 2 ), f (a, a 2 ) = a 2 = b 2 (x x 2 ) 2 = b 2 (a 2 4a 2 ), a = b 2 (a 2 4a 2), n whch, b s some ratonal functon of the coeffcents a, a 2. No other radcal a 2 of the frst order can enter nto the sought rreducble expresson for x; because the same reasonng would show that any such new radcal ought to be reducble to the form a 2 = c(x x 2 ) = c b a, 25

28 c beng some new symmetrc functon of the roots, and consequently some new ratonal functon of the coeffcents; so that, after calculatng the radcal a, t would be unnecessary to effect any new extracton of prme roots for the purpose of calculatng a 2, whch latter radcal would therefore be superfluous. Nor can any radcal a of hgher order enter, because such radcal would have 2α values, α beng greater than, whle any ratonal functon f, of two arbtrary quanttes x, x 2, can receve only two values, through any changes of ther arrangement. The exponent m, of the order of the sought rreducble functon b (m), must therefore be =, and ths functon tself must be of the form b = b 0 + b a, b 0 and b beng ratonal functons of a, a 2, or symmetrc functons of the two roots x, x 2, whch roots must admt of beng separately expressed as follows: x = b 0 + b a, x 2 = b 0 b a, f any expresson of the sought knd can be found for ether of them. It s, therefore, necessary and suffcent for the exstence of such an expresson, that the two followng quanttes, b 0 = x + x 2 2, b = x x 2 2a, should admt of beng expressed as ratonal functons of a, a 2 ; and ths condton s satsfed, snce the foregong relatons gve b 0 = a 2, b = 2b. We fnd, therefore, as the sought rratonal and rreducble expresson, and as the only possble expresson of that knd, (or at least as one wth whch all others must essentally concde,) for a root x of the general quadratc, the followng: x = b = a 2 + b 2b 2 (a 2 4a 2); b stll denotng any arbtrary ratonal functon of the two arbtrary coeffcents a, a 2, or any numercal constant, (such as the number 2, whch was the value of the quantty b n the formulæ of the precedng artcles,) and the two separate roots x, x 2, beng obtaned by takng separately the two sgns of the radcal. And thus we see à pror, that every method, for calculatng a root x of the general quadratc equaton as a functon of the two coeffcents, by any fnte number of addtons, subtractons, multplcatons, dvsons, elevatons to powers, and extractons of prme radcals, (these last extractons beng supposed to be reduced to the smallest possble number,) must nvolve the extracton of some one square-root of the form a = b 2 (a 2 4a 2), and must not nvolve the extracton of any other radcal. But ths square-root a s not essentally dstnct from that whch s usually assgned for the soluton of the general quadratc: t s therefore mpossble to dscover any new rratonal expresson, fnte and rreducble, for a root of that general quadratc, essentally dstnct from the expressons whch have long been known: and the only possble dfference between the extractons of radcals whch are requred n any two methods of soluton, f nether method requre any superfluous extracton, s that these methods may ntroduce dfferent square factors nto the expressons of that quantty or functon f, of whch, n each, the square root a s to be calculated. 26

Foundations of Arithmetic

Foundations of Arithmetic Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an

More information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could

More information

Module 9. Lecture 6. Duality in Assignment Problems

Module 9. Lecture 6. Duality in Assignment Problems Module 9 1 Lecture 6 Dualty n Assgnment Problems In ths lecture we attempt to answer few other mportant questons posed n earler lecture for (AP) and see how some of them can be explaned through the concept

More information

Difference Equations

Difference Equations Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1

More information

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens THE CHINESE REMAINDER THEOREM KEITH CONRAD We should thank the Chnese for ther wonderful remander theorem. Glenn Stevens 1. Introducton The Chnese remander theorem says we can unquely solve any par of

More information

a b a In case b 0, a being divisible by b is the same as to say that

a b a In case b 0, a being divisible by b is the same as to say that Secton 6.2 Dvsblty among the ntegers An nteger a ε s dvsble by b ε f there s an nteger c ε such that a = bc. Note that s dvsble by any nteger b, snce = b. On the other hand, a s dvsble by only f a = :

More information

The Order Relation and Trace Inequalities for. Hermitian Operators

The Order Relation and Trace Inequalities for. Hermitian Operators Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence

More information

Complex Numbers. x = B B 2 4AC 2A. or x = x = 2 ± 4 4 (1) (5) 2 (1)

Complex Numbers. x = B B 2 4AC 2A. or x = x = 2 ± 4 4 (1) (5) 2 (1) Complex Numbers If you have not yet encountered complex numbers, you wll soon do so n the process of solvng quadratc equatons. The general quadratc equaton Ax + Bx + C 0 has solutons x B + B 4AC A For

More information

8.6 The Complex Number System

8.6 The Complex Number System 8.6 The Complex Number System Earler n the chapter, we mentoned that we cannot have a negatve under a square root, snce the square of any postve or negatve number s always postve. In ths secton we want

More information

FINITELY-GENERATED MODULES OVER A PRINCIPAL IDEAL DOMAIN

FINITELY-GENERATED MODULES OVER A PRINCIPAL IDEAL DOMAIN FINITELY-GENERTED MODULES OVER PRINCIPL IDEL DOMIN EMMNUEL KOWLSKI Throughout ths note, s a prncpal deal doman. We recall the classfcaton theorem: Theorem 1. Let M be a fntely-generated -module. (1) There

More information

= z 20 z n. (k 20) + 4 z k = 4

= z 20 z n. (k 20) + 4 z k = 4 Problem Set #7 solutons 7.2.. (a Fnd the coeffcent of z k n (z + z 5 + z 6 + z 7 + 5, k 20. We use the known seres expanson ( n+l ( z l l z n below: (z + z 5 + z 6 + z 7 + 5 (z 5 ( + z + z 2 + z + 5 5

More information

Canonical transformations

Canonical transformations Canoncal transformatons November 23, 2014 Recall that we have defned a symplectc transformaton to be any lnear transformaton M A B leavng the symplectc form nvarant, Ω AB M A CM B DΩ CD Coordnate transformatons,

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

Section 3.6 Complex Zeros

Section 3.6 Complex Zeros 04 Chapter Secton 6 Comple Zeros When fndng the zeros of polynomals, at some pont you're faced wth the problem Whle there are clearly no real numbers that are solutons to ths equaton, leavng thngs there

More information

PHYS 705: Classical Mechanics. Calculus of Variations II

PHYS 705: Classical Mechanics. Calculus of Variations II 1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary

More information

More metrics on cartesian products

More metrics on cartesian products More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of

More information

Problem Solving in Math (Math 43900) Fall 2013

Problem Solving in Math (Math 43900) Fall 2013 Problem Solvng n Math (Math 43900) Fall 2013 Week four (September 17) solutons Instructor: Davd Galvn 1. Let a and b be two nteger for whch a b s dvsble by 3. Prove that a 3 b 3 s dvsble by 9. Soluton:

More information

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also

More information

Fundamental loop-current method using virtual voltage sources technique for special cases

Fundamental loop-current method using virtual voltage sources technique for special cases Fundamental loop-current method usng vrtual voltage sources technque for specal cases George E. Chatzaraks, 1 Marna D. Tortorel 1 and Anastasos D. Tzolas 1 Electrcal and Electroncs Engneerng Departments,

More information

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,

More information

Asymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation

Asymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation Nonl. Analyss and Dfferental Equatons, ol., 4, no., 5 - HIKARI Ltd, www.m-har.com http://dx.do.org/.988/nade.4.456 Asymptotcs of the Soluton of a Boundary alue Problem for One-Characterstc Dfferental Equaton

More information

Affine transformations and convexity

Affine transformations and convexity Affne transformatons and convexty The purpose of ths document s to prove some basc propertes of affne transformatons nvolvng convex sets. Here are a few onlne references for background nformaton: http://math.ucr.edu/

More information

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

COMPLEX NUMBERS AND QUADRATIC EQUATIONS COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not

More information

Example: (13320, 22140) =? Solution #1: The divisors of are 1, 2, 3, 4, 5, 6, 9, 10, 12, 15, 18, 20, 27, 30, 36, 41,

Example: (13320, 22140) =? Solution #1: The divisors of are 1, 2, 3, 4, 5, 6, 9, 10, 12, 15, 18, 20, 27, 30, 36, 41, The greatest common dvsor of two ntegers a and b (not both zero) s the largest nteger whch s a common factor of both a and b. We denote ths number by gcd(a, b), or smply (a, b) when there s no confuson

More information

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons

More information

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2 Salmon: Lectures on partal dfferental equatons 5. Classfcaton of second-order equatons There are general methods for classfyng hgher-order partal dfferental equatons. One s very general (applyng even to

More information

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0 MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector

More information

5 The Rational Canonical Form

5 The Rational Canonical Form 5 The Ratonal Canoncal Form Here p s a monc rreducble factor of the mnmum polynomal m T and s not necessarly of degree one Let F p denote the feld constructed earler n the course, consstng of all matrces

More information

Polynomials. 1 More properties of polynomials

Polynomials. 1 More properties of polynomials Polynomals 1 More propertes of polynomals Recall that, for R a commutatve rng wth unty (as wth all rngs n ths course unless otherwse noted), we defne R[x] to be the set of expressons n =0 a x, where a

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

SL n (F ) Equals its Own Derived Group

SL n (F ) Equals its Own Derived Group Internatonal Journal of Algebra, Vol. 2, 2008, no. 12, 585-594 SL n (F ) Equals ts Own Derved Group Jorge Macel BMCC-The Cty Unversty of New York, CUNY 199 Chambers street, New York, NY 10007, USA macel@cms.nyu.edu

More information

Advanced Quantum Mechanics

Advanced Quantum Mechanics Advanced Quantum Mechancs Rajdeep Sensarma! sensarma@theory.tfr.res.n ecture #9 QM of Relatvstc Partcles Recap of ast Class Scalar Felds and orentz nvarant actons Complex Scalar Feld and Charge conjugaton

More information

DIFFERENTIAL FORMS BRIAN OSSERMAN

DIFFERENTIAL FORMS BRIAN OSSERMAN DIFFERENTIAL FORMS BRIAN OSSERMAN Dfferentals are an mportant topc n algebrac geometry, allowng the use of some classcal geometrc arguments n the context of varetes over any feld. We wll use them to defne

More information

12. The Hamilton-Jacobi Equation Michael Fowler

12. The Hamilton-Jacobi Equation Michael Fowler 1. The Hamlton-Jacob Equaton Mchael Fowler Back to Confguraton Space We ve establshed that the acton, regarded as a functon of ts coordnate endponts and tme, satsfes ( ) ( ) S q, t / t+ H qpt,, = 0, and

More information

1 Generating functions, continued

1 Generating functions, continued Generatng functons, contnued. Exponental generatng functons and set-parttons At ths pont, we ve come up wth good generatng-functon dscussons based on 3 of the 4 rows of our twelvefold way. Wll our nteger-partton

More information

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity LINEAR REGRESSION ANALYSIS MODULE IX Lecture - 30 Multcollnearty Dr. Shalabh Department of Mathematcs and Statstcs Indan Insttute of Technology Kanpur 2 Remedes for multcollnearty Varous technques have

More information

NP-Completeness : Proofs

NP-Completeness : Proofs NP-Completeness : Proofs Proof Methods A method to show a decson problem Π NP-complete s as follows. (1) Show Π NP. (2) Choose an NP-complete problem Π. (3) Show Π Π. A method to show an optmzaton problem

More information

Errors for Linear Systems

Errors for Linear Systems Errors for Lnear Systems When we solve a lnear system Ax b we often do not know A and b exactly, but have only approxmatons  and ˆb avalable. Then the best thng we can do s to solve ˆx ˆb exactly whch

More information

THE SUMMATION NOTATION Ʃ

THE SUMMATION NOTATION Ʃ Sngle Subscrpt otaton THE SUMMATIO OTATIO Ʃ Most of the calculatons we perform n statstcs are repettve operatons on lsts of numbers. For example, we compute the sum of a set of numbers, or the sum of the

More information

Linear Algebra and its Applications

Linear Algebra and its Applications Lnear Algebra and ts Applcatons 4 (00) 5 56 Contents lsts avalable at ScenceDrect Lnear Algebra and ts Applcatons journal homepage: wwwelsevercom/locate/laa Notes on Hlbert and Cauchy matrces Mroslav Fedler

More information

Beyond Zudilin s Conjectured q-analog of Schmidt s problem

Beyond Zudilin s Conjectured q-analog of Schmidt s problem Beyond Zudln s Conectured q-analog of Schmdt s problem Thotsaporn Ae Thanatpanonda thotsaporn@gmalcom Mathematcs Subect Classfcaton: 11B65 33B99 Abstract Usng the methodology of (rgorous expermental mathematcs

More information

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1 C/CS/Phy9 Problem Set 3 Solutons Out: Oct, 8 Suppose you have two qubts n some arbtrary entangled state ψ You apply the teleportaton protocol to each of the qubts separately What s the resultng state obtaned

More information

Structure and Drive Paul A. Jensen Copyright July 20, 2003

Structure and Drive Paul A. Jensen Copyright July 20, 2003 Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.

More information

10. Canonical Transformations Michael Fowler

10. Canonical Transformations Michael Fowler 10. Canoncal Transformatons Mchael Fowler Pont Transformatons It s clear that Lagrange s equatons are correct for any reasonable choce of parameters labelng the system confguraton. Let s call our frst

More information

Graph Reconstruction by Permutations

Graph Reconstruction by Permutations Graph Reconstructon by Permutatons Perre Ille and Wllam Kocay* Insttut de Mathémathques de Lumny CNRS UMR 6206 163 avenue de Lumny, Case 907 13288 Marselle Cedex 9, France e-mal: lle@ml.unv-mrs.fr Computer

More information

The internal structure of natural numbers and one method for the definition of large prime numbers

The internal structure of natural numbers and one method for the definition of large prime numbers The nternal structure of natural numbers and one method for the defnton of large prme numbers Emmanul Manousos APM Insttute for the Advancement of Physcs and Mathematcs 3 Poulou str. 53 Athens Greece Abstract

More information

Solutions to the 71st William Lowell Putnam Mathematical Competition Saturday, December 4, 2010

Solutions to the 71st William Lowell Putnam Mathematical Competition Saturday, December 4, 2010 Solutons to the 7st Wllam Lowell Putnam Mathematcal Competton Saturday, December 4, 2 Kran Kedlaya and Lenny Ng A The largest such k s n+ 2 n 2. For n even, ths value s acheved by the partton {,n},{2,n

More information

MA 323 Geometric Modelling Course Notes: Day 13 Bezier Curves & Bernstein Polynomials

MA 323 Geometric Modelling Course Notes: Day 13 Bezier Curves & Bernstein Polynomials MA 323 Geometrc Modellng Course Notes: Day 13 Bezer Curves & Bernsten Polynomals Davd L. Fnn Over the past few days, we have looked at de Casteljau s algorthm for generatng a polynomal curve, and we have

More information

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Physics 5153 Classical Mechanics. Principle of Virtual Work-1 P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal

More information

Remarks on the Properties of a Quasi-Fibonacci-like Polynomial Sequence

Remarks on the Properties of a Quasi-Fibonacci-like Polynomial Sequence Remarks on the Propertes of a Quas-Fbonacc-lke Polynomal Sequence Brce Merwne LIU Brooklyn Ilan Wenschelbaum Wesleyan Unversty Abstract Consder the Quas-Fbonacc-lke Polynomal Sequence gven by F 0 = 1,

More information

FREQUENCY DISTRIBUTIONS Page 1 of The idea of a frequency distribution for sets of observations will be introduced,

FREQUENCY DISTRIBUTIONS Page 1 of The idea of a frequency distribution for sets of observations will be introduced, FREQUENCY DISTRIBUTIONS Page 1 of 6 I. Introducton 1. The dea of a frequency dstrbuton for sets of observatons wll be ntroduced, together wth some of the mechancs for constructng dstrbutons of data. Then

More information

ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION

ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION Advanced Mathematcal Models & Applcatons Vol.3, No.3, 2018, pp.215-222 ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EUATION

More information

2.3 Nilpotent endomorphisms

2.3 Nilpotent endomorphisms s a block dagonal matrx, wth A Mat dm U (C) In fact, we can assume that B = B 1 B k, wth B an ordered bass of U, and that A = [f U ] B, where f U : U U s the restrcton of f to U 40 23 Nlpotent endomorphsms

More information

BOUNDEDNESS OF THE RIESZ TRANSFORM WITH MATRIX A 2 WEIGHTS

BOUNDEDNESS OF THE RIESZ TRANSFORM WITH MATRIX A 2 WEIGHTS BOUNDEDNESS OF THE IESZ TANSFOM WITH MATIX A WEIGHTS Introducton Let L = L ( n, be the functon space wth norm (ˆ f L = f(x C dx d < For a d d matrx valued functon W : wth W (x postve sem-defnte for all

More information

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016 U.C. Berkeley CS94: Spectral Methods and Expanders Handout 8 Luca Trevsan February 7, 06 Lecture 8: Spectral Algorthms Wrap-up In whch we talk about even more generalzatons of Cheeger s nequaltes, and

More information

CHAPTER 5: Lie Differentiation and Angular Momentum

CHAPTER 5: Lie Differentiation and Angular Momentum CHAPTER 5: Le Dfferentaton and Angular Momentum Jose G. Vargas 1 Le dfferentaton Kähler s theory of angular momentum s a specalzaton of hs approach to Le dfferentaton. We could deal wth the former drectly,

More information

Bezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0

Bezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0 Bezer curves Mchael S. Floater August 25, 211 These notes provde an ntroducton to Bezer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of the

More information

CHAPTER 14 GENERAL PERTURBATION THEORY

CHAPTER 14 GENERAL PERTURBATION THEORY CHAPTER 4 GENERAL PERTURBATION THEORY 4 Introducton A partcle n orbt around a pont mass or a sphercally symmetrc mass dstrbuton s movng n a gravtatonal potental of the form GM / r In ths potental t moves

More information

Bernoulli Numbers and Polynomials

Bernoulli Numbers and Polynomials Bernoull Numbers and Polynomals T. Muthukumar tmk@tk.ac.n 17 Jun 2014 The sum of frst n natural numbers 1, 2, 3,..., n s n n(n + 1 S 1 (n := m = = n2 2 2 + n 2. Ths formula can be derved by notng that

More information

Week 2. This week, we covered operations on sets and cardinality.

Week 2. This week, we covered operations on sets and cardinality. Week 2 Ths week, we covered operatons on sets and cardnalty. Defnton 0.1 (Correspondence). A correspondence between two sets A and B s a set S contaned n A B = {(a, b) a A, b B}. A correspondence from

More information

Invariant variational problems

Invariant variational problems Invarante Varatonsprobleme, Kgl. Ges. d. Wss. Nachrchten, Math.-phys. Klasse (1918), 235-257. Invarant varatonal problems (F. Klen on hs ffty-year Doctoral Jublee) By Emmy Noether n Göttngen. (Presented

More information

where a is any ideal of R. Lemma 5.4. Let R be a ring. Then X = Spec R is a topological space Moreover the open sets

where a is any ideal of R. Lemma 5.4. Let R be a ring. Then X = Spec R is a topological space Moreover the open sets 5. Schemes To defne schemes, just as wth algebrac varetes, the dea s to frst defne what an affne scheme s, and then realse an arbtrary scheme, as somethng whch s locally an affne scheme. The defnton of

More information

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 3, Issue 1, July 2013

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 3, Issue 1, July 2013 ISSN: 2277-375 Constructon of Trend Free Run Orders for Orthogonal rrays Usng Codes bstract: Sometmes when the expermental runs are carred out n a tme order sequence, the response can depend on the run

More information

Math 261 Exercise sheet 2

Math 261 Exercise sheet 2 Math 261 Exercse sheet 2 http://staff.aub.edu.lb/~nm116/teachng/2017/math261/ndex.html Verson: September 25, 2017 Answers are due for Monday 25 September, 11AM. The use of calculators s allowed. Exercse

More information

Problem Do any of the following determine homomorphisms from GL n (C) to GL n (C)?

Problem Do any of the following determine homomorphisms from GL n (C) to GL n (C)? Homework 8 solutons. Problem 16.1. Whch of the followng defne homomomorphsms from C\{0} to C\{0}? Answer. a) f 1 : z z Yes, f 1 s a homomorphsm. We have that z s the complex conjugate of z. If z 1,z 2

More information

arxiv: v1 [math.ho] 18 May 2008

arxiv: v1 [math.ho] 18 May 2008 Recurrence Formulas for Fbonacc Sums Adlson J. V. Brandão, João L. Martns 2 arxv:0805.2707v [math.ho] 8 May 2008 Abstract. In ths artcle we present a new recurrence formula for a fnte sum nvolvng the Fbonacc

More information

PRIMES 2015 reading project: Problem set #3

PRIMES 2015 reading project: Problem set #3 PRIMES 2015 readng project: Problem set #3 page 1 PRIMES 2015 readng project: Problem set #3 posted 31 May 2015, to be submtted around 15 June 2015 Darj Grnberg The purpose of ths problem set s to replace

More information

( ) 2 ( ) ( ) Problem Set 4 Suggested Solutions. Problem 1

( ) 2 ( ) ( ) Problem Set 4 Suggested Solutions. Problem 1 Problem Set 4 Suggested Solutons Problem (A) The market demand functon s the soluton to the followng utlty-maxmzaton roblem (UMP): The Lagrangean: ( x, x, x ) = + max U x, x, x x x x st.. x + x + x y x,

More information

Linear, affine, and convex sets and hulls In the sequel, unless otherwise specified, X will denote a real vector space.

Linear, affine, and convex sets and hulls In the sequel, unless otherwise specified, X will denote a real vector space. Lnear, affne, and convex sets and hulls In the sequel, unless otherwse specfed, X wll denote a real vector space. Lnes and segments. Gven two ponts x, y X, we defne xy = {x + t(y x) : t R} = {(1 t)x +

More information

The Feynman path integral

The Feynman path integral The Feynman path ntegral Aprl 3, 205 Hesenberg and Schrödnger pctures The Schrödnger wave functon places the tme dependence of a physcal system n the state, ψ, t, where the state s a vector n Hlbert space

More information

The exponential map of GL(N)

The exponential map of GL(N) The exponental map of GLN arxv:hep-th/9604049v 9 Apr 996 Alexander Laufer Department of physcs Unversty of Konstanz P.O. 5560 M 678 78434 KONSTANZ Aprl 9, 996 Abstract A fnte expanson of the exponental

More information

where a is any ideal of R. Lemma Let R be a ring. Then X = Spec R is a topological space. Moreover the open sets

where a is any ideal of R. Lemma Let R be a ring. Then X = Spec R is a topological space. Moreover the open sets 11. Schemes To defne schemes, just as wth algebrac varetes, the dea s to frst defne what an affne scheme s, and then realse an arbtrary scheme, as somethng whch s locally an affne scheme. The defnton of

More information

Polynomial Regression Models

Polynomial Regression Models LINEAR REGRESSION ANALYSIS MODULE XII Lecture - 6 Polynomal Regresson Models Dr. Shalabh Department of Mathematcs and Statstcs Indan Insttute of Technology Kanpur Test of sgnfcance To test the sgnfcance

More information

Société de Calcul Mathématique SA

Société de Calcul Mathématique SA Socété de Calcul Mathématque SA Outls d'ade à la décson Tools for decson help Probablstc Studes: Normalzng the Hstograms Bernard Beauzamy December, 202 I. General constructon of the hstogram Any probablstc

More information

Polynomials. 1 What is a polynomial? John Stalker

Polynomials. 1 What is a polynomial? John Stalker Polynomals John Stalker What s a polynomal? If you thnk you already know what a polynomal s then skp ths secton. Just be aware that I consstently wrte thngs lke p = c z j =0 nstead of p(z) = c z. =0 You

More information

Formulas for the Determinant

Formulas for the Determinant page 224 224 CHAPTER 3 Determnants e t te t e 2t 38 A = e t 2te t e 2t e t te t 2e 2t 39 If 123 A = 345, 456 compute the matrx product A adj(a) What can you conclude about det(a)? For Problems 40 43, use

More information

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential Open Systems: Chemcal Potental and Partal Molar Quanttes Chemcal Potental For closed systems, we have derved the followng relatonshps: du = TdS pdv dh = TdS + Vdp da = SdT pdv dg = VdP SdT For open systems,

More information

A new construction of 3-separable matrices via an improved decoding of Macula s construction

A new construction of 3-separable matrices via an improved decoding of Macula s construction Dscrete Optmzaton 5 008 700 704 Contents lsts avalable at ScenceDrect Dscrete Optmzaton journal homepage: wwwelsevercom/locate/dsopt A new constructon of 3-separable matrces va an mproved decodng of Macula

More information

9 Characteristic classes

9 Characteristic classes THEODORE VORONOV DIFFERENTIAL GEOMETRY. Sprng 2009 [under constructon] 9 Characterstc classes 9.1 The frst Chern class of a lne bundle Consder a complex vector bundle E B of rank p. We shall construct

More information

18.781: Solution to Practice Questions for Final Exam

18.781: Solution to Practice Questions for Final Exam 18.781: Soluton to Practce Questons for Fnal Exam 1. Fnd three solutons n postve ntegers of x 6y = 1 by frst calculatng the contnued fracton expanson of 6. Soluton: We have 1 6=[, ] 6 6+ =[, ] 1 =[,, ]=[,,

More information

Chapter 13: Multiple Regression

Chapter 13: Multiple Regression Chapter 13: Multple Regresson 13.1 Developng the multple-regresson Model The general model can be descrbed as: It smplfes for two ndependent varables: The sample ft parameter b 0, b 1, and b are used to

More information

8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS

8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS SECTION 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS 493 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS All the vector spaces you have studed thus far n the text are real vector spaces because the scalars

More information

Perron Vectors of an Irreducible Nonnegative Interval Matrix

Perron Vectors of an Irreducible Nonnegative Interval Matrix Perron Vectors of an Irreducble Nonnegatve Interval Matrx Jr Rohn August 4 2005 Abstract As s well known an rreducble nonnegatve matrx possesses a unquely determned Perron vector. As the man result of

More information

On the set of natural numbers

On the set of natural numbers On the set of natural numbers by Jalton C. Ferrera Copyrght 2001 Jalton da Costa Ferrera Introducton The natural numbers have been understood as fnte numbers, ths wor tres to show that the natural numbers

More information

1 GSW Iterative Techniques for y = Ax

1 GSW Iterative Techniques for y = Ax 1 for y = A I m gong to cheat here. here are a lot of teratve technques that can be used to solve the general case of a set of smultaneous equatons (wrtten n the matr form as y = A), but ths chapter sn

More information

ANSWERS. Problem 1. and the moment generating function (mgf) by. defined for any real t. Use this to show that E( U) var( U)

ANSWERS. Problem 1. and the moment generating function (mgf) by. defined for any real t. Use this to show that E( U) var( U) Econ 413 Exam 13 H ANSWERS Settet er nndelt 9 deloppgaver, A,B,C, som alle anbefales å telle lkt for å gøre det ltt lettere å stå. Svar er gtt . Unfortunately, there s a prntng error n the hnt of

More information

Solution Thermodynamics

Solution Thermodynamics Soluton hermodynamcs usng Wagner Notaton by Stanley. Howard Department of aterals and etallurgcal Engneerng South Dakota School of nes and echnology Rapd Cty, SD 57701 January 7, 001 Soluton hermodynamcs

More information

2E Pattern Recognition Solutions to Introduction to Pattern Recognition, Chapter 2: Bayesian pattern classification

2E Pattern Recognition Solutions to Introduction to Pattern Recognition, Chapter 2: Bayesian pattern classification E395 - Pattern Recognton Solutons to Introducton to Pattern Recognton, Chapter : Bayesan pattern classfcaton Preface Ths document s a soluton manual for selected exercses from Introducton to Pattern Recognton

More information

The KMO Method for Solving Non-homogenous, m th Order Differential Equations

The KMO Method for Solving Non-homogenous, m th Order Differential Equations The KMO Method for Solvng Non-homogenous, m th Order Dfferental Equatons Davd Krohn Danel Marño-Johnson John Paul Ouyang March 14, 2013 Abstract Ths paper shows a smple tabular procedure for fndng the

More information

ALGEBRA HW 7 CLAY SHONKWILER

ALGEBRA HW 7 CLAY SHONKWILER ALGEBRA HW 7 CLAY SHONKWILER 1 Whch of the followng rngs R are dscrete valuaton rngs? For those that are, fnd the fracton feld K = frac R, the resdue feld k = R/m (where m) s the maxmal deal), and a unformzer

More information

Affine and Riemannian Connections

Affine and Riemannian Connections Affne and Remannan Connectons Semnar Remannan Geometry Summer Term 2015 Prof Dr Anna Wenhard and Dr Gye-Seon Lee Jakob Ullmann Notaton: X(M) space of smooth vector felds on M D(M) space of smooth functons

More information

CALCULUS CLASSROOM CAPSULES

CALCULUS CLASSROOM CAPSULES CALCULUS CLASSROOM CAPSULES SESSION S86 Dr. Sham Alfred Rartan Valley Communty College salfred@rartanval.edu 38th AMATYC Annual Conference Jacksonvlle, Florda November 8-, 202 2 Calculus Classroom Capsules

More information

Lecture 10 Support Vector Machines II

Lecture 10 Support Vector Machines II Lecture 10 Support Vector Machnes II 22 February 2016 Taylor B. Arnold Yale Statstcs STAT 365/665 1/28 Notes: Problem 3 s posted and due ths upcomng Frday There was an early bug n the fake-test data; fxed

More information

On the correction of the h-index for career length

On the correction of the h-index for career length 1 On the correcton of the h-ndex for career length by L. Egghe Unverstet Hasselt (UHasselt), Campus Depenbeek, Agoralaan, B-3590 Depenbeek, Belgum 1 and Unverstet Antwerpen (UA), IBW, Stadscampus, Venusstraat

More information

A how to guide to second quantization method.

A how to guide to second quantization method. Phys. 67 (Graduate Quantum Mechancs Sprng 2009 Prof. Pu K. Lam. Verson 3 (4/3/2009 A how to gude to second quantzaton method. -> Second quantzaton s a mathematcal notaton desgned to handle dentcal partcle

More information

THERE ARE NO POINTS OF ORDER 11 ON ELLIPTIC CURVES OVER Q.

THERE ARE NO POINTS OF ORDER 11 ON ELLIPTIC CURVES OVER Q. THERE ARE NO POINTS OF ORDER 11 ON ELLIPTIC CURVES OVER Q. IAN KIMING We shall prove the followng result from [2]: Theorem 1. (Bllng-Mahler, 1940, cf. [2]) An ellptc curve defned over Q does not have a

More information

763622S ADVANCED QUANTUM MECHANICS Solution Set 1 Spring c n a n. c n 2 = 1.

763622S ADVANCED QUANTUM MECHANICS Solution Set 1 Spring c n a n. c n 2 = 1. 7636S ADVANCED QUANTUM MECHANICS Soluton Set 1 Sprng 013 1 Warm-up Show that the egenvalues of a Hermtan operator  are real and that the egenkets correspondng to dfferent egenvalues are orthogonal (b)

More information

Bézier curves. Michael S. Floater. September 10, These notes provide an introduction to Bézier curves. i=0

Bézier curves. Michael S. Floater. September 10, These notes provide an introduction to Bézier curves. i=0 Bézer curves Mchael S. Floater September 1, 215 These notes provde an ntroducton to Bézer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of

More information

Workshop: Approximating energies and wave functions Quantum aspects of physical chemistry

Workshop: Approximating energies and wave functions Quantum aspects of physical chemistry Workshop: Approxmatng energes and wave functons Quantum aspects of physcal chemstry http://quantum.bu.edu/pltl/6/6.pdf Last updated Thursday, November 7, 25 7:9:5-5: Copyrght 25 Dan Dll (dan@bu.edu) Department

More information