What is Orbital Angular Momentum?

Transcription

1 What is Orbital Angular Momentum? Matthias Burkardt New Mexico State University & Jefferson Lab What is Orbital Angular Momentum? p.1/23

2 Motivation polarized DIS: only 30% of the proton spin due to quark spins spin crisis spin puzzle, because Σ much smaller than the quark model result Σ = 1 quest for the remaining 70% quark orbital angular momentum OAM) gluon spin gluon OAM How are the above quantities defined? How can the above quantities be measured What is Orbital Angular Momentum? p.2/23

3 example: angular momentum in QED consider, for simplicity, QED without electrons: J = ) d 3 r x E B = [ )] d 3 r x E A integrate by parts J = d 3 r [ E j x ) A j + x A ) ] E + E A drop 2 nd term eq. of motion E = 0), yielding J = L + S with L = ) d 3 r E j x A j S = d 3 r E A note: L and S not separately gauge invariant What is Orbital Angular Momentum? p.3/23

4 example cont.) total angular momentum of isolated system uniquely defined ambiguities arise when decomposing J into contributions from different constituents gauge theories: changing gauge may also shift angular momentum between various degrees of freedom decomposition of angular momentum in general depends on scheme gauge & quantization scheme) does not mean that angular momentum decomposition is meaningless, but one needs to be aware of this scheme -dependence in the physical interpretation of exp/lattice/model results in terms of spin vs. OAM and, for example, not mix schemes, e.t.c. What is Orbital Angular Momentum? p.4/23

5 Outline Ji decomposition Jaffe decomposition recent lattice results Ji decomposition) model/qed illustrations for Ji v. Jaffe What is Orbital Angular Momentum? p.5/23

6 The nucleon spin pizzas) Ji Jaffe & Manohar L q 1 2 Σ 1 L q 2 Σ J g L g G pizza tre stagioni pizza quattro stagioni only 1 2 Σ 1 2 q q common to both decompositions! What is Orbital Angular Momentum? p.6/23

7 Ji-decomposition L q 1 2 Σ Ji 1997) 1 2 = q J q + J g = q ) 1 2 q + L q + J g J g with P µ = M, 0, 0, 1), S µ = 0, 0, 0, 1)) 1 2 q = 1 d 3 x P, S q x)σ 3 q x) P, S Σ 3 = iγ 1 γ 2 2 L q = d 3 x P, S q x) x id) 3 q x) P, S [ 3 J g = d 3 x P, S x E B)] P, S i D = i g A What is Orbital Angular Momentum? p.7/23

8 Ji-decomposition L q J = q 1 2 q Σq + q r id ) q + r E B ) applies to each vector component of nucleon angular momentum, but Ji-decomposition usually applied only to ẑ component where at least quark spin has parton interpretation as difference between number densities q from polarized DIS J q = 1 2 q + L q from exp/lattice GPDs) J g 1 2 Σ L q in principle independently defined as matrix elements of ) q r i D q, but in practice easier by subtraction L q = J q 1 2 q J g in principle accessible through gluon GPDs, but in practice easier by subtraction J g = 1 2 L q further decomposition of J g into intrinsic spin) and extrinsic OAM) that is local and manifestly gauge invariant has not been found What is Orbital Angular Momentum? p.8/23

9 L q for proton from Ji-relation lattice) lattice QCD moments of GPDs Negele++; Schierholz++) insert in Ji-relation J i q = S i dx[h q x, 0) + E q x, 0)] x. L z q = J z q 1 2 q L u, L d both large! present calcs. show L u + L d 0, but disconnected diagrams..? m 2 π extrapolation parton interpret. of L q... What is Orbital Angular Momentum? p.9/23

10 Jaffe/Manohar decomposition in light-cone framework & light-cone gauge A + = 0 one finds for J z = dx d 2 r M +xy q L q L g G 1 2 Σ 1 2 = 1 2 Σ + q L q + G + L g where γ + = γ 0 + γ z ) L q = d 3 r P, S q r)γ + r i ) z q r) P, S G = ε + ij d 3 r P, S TrF +i A j P, S L g = 2 d 3 r P, S TrF +j x i ) z A j P, S What is Orbital Angular Momentum? p.10/23

11 Jaffe/Manohar decomposition Σ = q 1 2 = 1 2 Σ + q L q + G + L g q from polarized DIS or lattice) q L q L g G 1 2 Σ G from p p or polarized DIS evolution) G gauge invariant, but local operator only in light-cone gauge dxx n Gx) for n 1 can be described by manifestly gauge inv. local op. lattice) L q, L g independently defined, but no exp. identified to access them not accessible on lattice, since nonlocal except when A + = 0 parton net OAM L = L g + q L q by subtr. L = Σ G in general, L q L q L g + G J g makes no sense to mix Ji and JM decompositions, e.g. J g G has no fundamental connection to OAM What is Orbital Angular Momentum? p.11/23

12 L q L q L q matrix element of q [ r i g A)] 3 q = qγ 0 [ r i g A)] 3 q L z q matrix element of γ + = γ 0 + γ z ) [ qγ + r i ] z q A+=0 For nucleon at rest, matrix element of L q same as that of qγ [ r + i g A)] z q even in light-cone gauge, L z q and L z q still differ by matrix element of q r g A) z q A + =0 = q xga y yga x ) q A + =0 What is Orbital Angular Momentum? p.12/23

13 Summary part 1: Ji: J z = 1 2 Σ + q L q + J g Jaffe: J z = 1 2 Σ + q L q + G + L g G can be defined without reference to gauge and hence gauge invariantly) as the quantity that enters the evolution equations and/or p p represented by simple i.e. local) operator only in LC gauge and corresponds to the operator that one would naturally identify with spin only in that gauge in general L q L q or J g G + L g, but how significant is the difference between L q and L q, etc.? What is Orbital Angular Momentum? p.13/23

14 OAM in scalar diquark model toy model for nucleon where nucleon mass M) splits into quark mass m) and scalar diquark mass λ) light-cone wave function for quark-diquark Fock component ψ x,k ) = M + m x ) φ ψ 1 2 = k1 + ik 2 x φ with φ = c/ 1 x M 2 k2 +m2 x k2 +λ2 1 x. quark OAM according to JM: L q = 1 0 dx d 2 k 16π 3 1 x) ψ 1 2 quark OAM according to Ji: L q = dxx[qx) + Ex, 0, 0)] 1 2 q using Lorentz inv. regularization, such as Pauli Villars subtraction) both give identical result, i.e. L q = L q not surprising since scalar diquark model is not a gauge theory 2 What is Orbital Angular Momentum? p.14/23

15 OAM in scalar diquark model But, even though L q = L q in this non-gauge theory L q x) d 2 k ψ 16π 3 1 x) {x[qx) + Ex, 0, 0)] qx)} L qx) 0.2 L x) 0.15 L x) x unintegrated Ji-relation does not yield x-distribution of OAM What is Orbital Angular Momentum? p.15/23

16 OAM in QED light-cone wave function in eγ Fock component Ψ + 1+1x,k ) = 2 k1 ik 2 2 x1 x) φ Ψ + 1 1x,k ) = 2 k1 + ik x Ψ 1+1x,k ) = m ) 2 2 x m φ Ψ 1+1x,k ) = 0 2 OAM of e according to Jaffe/Manohar L e = 1 0 dx d 2 k [1 x) Ψ + 1 1x,k ) 2 2 Ψ + 1+1x,k ) 2 2] e OAM according to Ji L e = dxx[qx) + Ex, 0, 0)] 1 2 q L e = L e + α 4π L e Likewise, computing J γ from photon GPD, and γ and L γ from light-cone wave functions yields L γ J γ γ = L γ + α 4π α 4π appears to be small, but L e, L e are all of O α π ) What is Orbital Angular Momentum? p.16/23

17 OAM in QCD 1-loop QCD: L q L q = α s 3π recall lattice QCD): L u.15; L d +.15 QCD evolution yields negative correction to L u and positive correction to L d evolution suggested A.W.Thomas) to explain apparent discrepancy between quark models low Q 2 ) and lattice results Q 2 4GeV 2 ) above result suggests that L u > L u and L d > L d additional contribution with same sign) from vector potential due to spectators MB, to be published) possible that lattice result consistent with L u > L d What is Orbital Angular Momentum? p.17/23

18 Summary polarized DIS provides access to quark spin 1 2 q gluon spin G parton grand total OAM L L g + q L q = 1 2 G q q DVCS & polarized DIS and/or lattice provide access to quark spin 1 2 q J q & L q = J q 1 2 q J g = 1 2 q J q J g G does not yield gluon OAM L q L q = O0.1) What is Orbital Angular Momentum? p.18/23

19 Announcement: workshop on Orbital Angular Momentum of Partons in Hadrons ECT 9-13 November 2009 organizers: M.B. & Gunar Schnell confirmed participants: M.Anselmino, H.Avakian, A.Bachetta, L.Bland, D.Boer, S.J.Brodksy, M.Diehl, D.Fields, L.Gamberg, G.Goldstein, M.Grosse-Perdekamp, P.Hägler, X.Ji, R.Kaiser, E.Leader, N.Makins, A.Miller, D.Müller, P.Mulders, A.Schäfer, G.Schierholz, O.Teryaev, W.Vogelsang, F.Yuan What is Orbital Angular Momentum? p.19/23