Diamond platforms for nanoscale photonics and metrology
|
|
|
- Randell Anthony
- 5 years ago
- Views:
Transcription
1 Diamond platforms for nanoscale photonics and metrology The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Shields, Brendan John Diamond platforms for nanoscale photonics and metrology. Doctoral dissertation, Harvard University. Citable link Terms of Use This article was downloaded from Harvard University s DASH repository, and is made available under the terms and conditions applicable to Other Posted Material, as set forth at nrs.harvard.edu/urn-3:hul.instrepos:dash.current.terms-ofuse#laa
2
3
4
5
6
7
8 594
9
10
11
12
13
14
15
16
17
18 0 637 m s =0 m s = ±1 2.8 m s = ±1 m s =0 m s =1 m s = ±1 m s = ±1 150 m s = 0 m s = 1 m s =0
19
20 532 m s =0 V Q V (λ/n) 3 λ n
21 2π 15
22 2π Q n = 2.4 Q
23
24
25
26 V m 1/ V m Q ΓX
27 air 0.3 light -lines PMMA e d waveguide bands bandgap X J k a// x E Air 2 z(+m) ï 1 1 b 1 5+m f 4 Target NV N h(nm) g.. onto substrate. 30+m 1+m 0.2..to polymer.. GaP wafer.. intensity (a.u.) normalized frequency a/h a V PC tip 0 film 1 PMMA c glass y(+m) ï 0 excitation & collection ï ï 0 x(+m) 6B;m`2 kxr, U V.BbT2`bBQM 7Q` i?2 T?QiQMB+ +`vbi H bh # BM B`- HQM; i?2 r p2;mb/2 /B`2+iBQM kx c i?2 BMb2i b?qrb i?2 +`vbi H UQ` M;2V M/ BMp2`b2 +`vbi H U#Hm2V /B`2+iBQMbX h?2 H iib+2? b T2`B@ Q/B+Biv Q7 a = 176MK-?QH2 ` /Bmb Q7 53 MK- M/ bh #?2B;?i Q7 110 MKX U#V 1M2`;v /2MbBiv 7Q` 7mM/ K2Mi H KQ/2 BM +`Qbb@b2+iBQM M/ U+V BM TH M2X U/V a1jx U2V h?2 T?QiQMB+ +`vbi Hb `2 i` Mb72``2/ 7`QK i?2 : S +?BT QMiQ bm#bi` i2 pb TQHvK2` bi KTX U7V "`Q /@# M/ `2~2+iBpBiv K2 bm`2k2mi Q7 + pbiv `2bQM M+2 rbi? Q X U;V h?2 S* bh # Bb TQbBiBQM2/ `2H ibp2 iq i `;2i M MQ+`vbi H BM i?2 TQHvK2` }HKX Rk
28 n s 1.5 Q V m =0.74(λ/n ) 3 n =3.4 λ = Q Q 30
29 a y(µm) b PL reflection x(µm) NV c 100 cts/s/nm 100 cts/s/nm cavity and NV d 4 2 I 0 I cb fits I c 2 2 (2) g (t ) 1 (2) g (t ) λ(nm) t (ns) t (ns) intensity (a.u.) e f uncoupled, τ =16.4 ±1.1 ns 0 coupled, τ =12.7 ± 1.2 ns c t(ns) I 0 I cb I c f c (λ 2 ) = 5.3,f c (λ 1 ) =
30 λ 1 = λ 2 = Q 1 = 550 Q 2 = I I c I cb
31 τ 0,c = 16.4 ± 1.1, 12.7 ± 1.5 F (λ) F (λ) =I c (λ)τ 0 /I 0 (λ)τ c F (λ 1 )=2.2 F (λ 2 ) 7.0 F (λ) a 180 S d (ω, r) =C NV + C cav f c ( r ) L(ω) 2 +2C int R[e i φ f c ( r )L(ω)], C NV C cav C int L(ω) =1/(1 + i(ω ω c )/κ) ω c κ = ω c /2Q φ
32 a target NV b c e target NV 4 µm scanning tip x d 1 µm PL reflection 680 λ λ 2 f PL λ(nm) fits x(nm) g experiment c f (λ, x x+ y ^ y) ^ 1 slip theory 0.3 y(µm) 0 y(nm) 0.3 c ^ h f (λ, x x+ y ^ y-98 ^ o 1 nm z, 20 ) x(nm) x = 3.4 f c (λ 1, r) 80 f c (λ 1, r) z = 98 ± 5 y = 70 ± 5 µ x
33 f c (ω, r) C NV C cav C int C NV C cav C int C int =0 f c (λ = 643, r)=5.3,f c (667, r)=0.7 S d (ω, r) f c (ω 1, r) ω 1 =2πc/λ 1 f c (ω 1, r) µ z = 98 ± 5 20 x x 190
34
35
36
37
38 Q 7 23
39 n =2.4
40 Q Q
41 T Q 2 Tot /Q2 wg Q Q scat Q Q wg Q Q Tot (λ/n) 3 Q Q scat = <Q wg 3.7(λ/n) 3 Q
42 Q Q Q
43 532 g 2 (0) =
44 23 7 Q
45 23
46 Q Q
47 F P 7
48 F P = 3 4π 2 ( ) λ 3 Q n V E NV µ NV 2 E max 2 µ NV 2, E NV,max µ NV λ n = 2.4 V = [ ɛ( r ) E( r ) d r] 2 /max [ɛ( r ) E( r ] ) I res ZPL =(η cav F P + η NV ) 1 τ 0, η cav,nv τ 0
49 F P =0 I off res ZPL = η NV F NV τ 0. η cav = η NV Q ZPL I off res ZPL χ = η cavf P η N V = Ires 1. χ Q 3.7 (λ/n) 3 Q Q 23 7
50 Q 10 3
51 0 0
52 0 m s =
53
54 n diamond n glass 532 m s = ±1 25 m s =0 m s =1
55 g 1 g 0 0 γ 0 γ 1 F C g 0,1 γ 0,
56 594 0 γ 1 γ 0 g 1 g µ γ 0,γ 1,g 0,g 1 594
57 15 t tg 1 1 P t R F C (P ) F C 0.9 µ t probe = g 1 t probe 1 t R = ± 0.006
58 0.975 ± p s =0.216 ± m s =1 m s =0 594 m s = 1 m s = m s =0 m s =
59 ± p s =0.216 ± ±
60 m s =0 m s = m s =0 0 m s = m s = ± m s = ±
61 m s = 0 m s =1 β 0 β 1 β 0 β 1 β 0,1 β 0,1 20 β 0,1 m s =1 β 1 60 δb = π τ + ti + t R σ R 2gµ B T τ 2, g µ B τ t I t R T N τ + t I + t R σ R
62 σ R t R m s =0 m s = t R σ R (t R ) = a 1+b/t 1/4 R a b t R σ R (t R ) σ R (t R ) (τ + t I + t R )/τ 2 t I 6.5 t I =1.5/p s p s =0.200 ± 0.006
63 σ R =1 τ α 0,1 m s =0, 1 σ trad R = 1+ 2(α 0 + α 1 ) (α 0 α 1 ) 2 σ trad R α 0 20 = ± α 1 =0.154 ± σ trad R = 10.6 ± 0.3 σ SCC R = (β 0 + β 1 )(2 β 0 β 1 ) (β 0 β 1 ) 2.
64 β 0,1 σ SCC R,best =2.76 ± 0.09 σr SCC (t R ) 6.5 t R σr SCC (t R ) β 0,1 t R σr SCC (t R ) t R 5 σr SCC (t R ) σr SCC (t R ) σr SCC (t R ) σ SCC R,best (t R) δb T = π τ + 2gµ ti + t R σscc R (t R ) τ 2
65 t R σr SCC (t R ) t R = /2 0
66
67 Q 10 5 Q
68
69
70 N j λ j γ j γ NR r i p i j I ij = cp i η ij γ ij k γ ik + γ NR = cp i η ij γ ij Γ i
71 η ij Γ i = k γ ik + γ NR c β ij = γ ij /Γ i j Γ i =1/τ i i 0 I ij I 0j = p iη ij γ ij Γ 0 p 0 η 0j γ 0j Γ i I ij I 0j = γ ijγ 0 γ 0j Γ i = F ij Γ 0 Γ i, F ij = γ ij /γ 0j = I ij Γ i /I 0j Γ 0 i =1 F 1j = F (λ j )
72 a b 80 cts/s/nm cts/s/nm 2 uncoupled NV uncoupled cav. 1 coupled NV/cav. fits x(nm) c Scan over NV centre λ(nm) fit λ(nm) C int =0.6 x 1 x 2 x x 1 λ 1 λ 2 λ 2
73 F(λ) λ(nm) F (λ)
74 a.1 λ 2 pump a.2 λ 2 a.3 λ 1, y-polarized, x-polarized, y-polarized y x(nm) x(nm) x1 x2 b c degrees λ 2 λ 1 collection from x2 collection from x λ(nm) d intensity (cts/s/nm) λ(nm) λ 1
75 C int = 0.6 = 2.87 m s = 0 m s = ±1 m s = ±1 m s = ±1 m s =0 m s = ±1
76 (2) g (τ) τ(ns)
77 Luminescence intensity (a.u.) 7 (a) Luminescence intensity (a.u.) (b) ν(ghz) microwave frequency t(ns) microwave pulse duration ν ν =2.77 ν m s =0 t ν =2.77 σ = g e a H = 2 a a 2 (σ z)+ig(σa aσ ),
78 dρ dt = i[h, ρ]+κ 2 (2aρa a aρ ρa a)+ γ 2 (2σρσ σ σρ ρσ σ)+ γ d 2 (σ zρσ z ρ) γ κ γ d σ z =[σ,σ] g, e 0, 1. da =( i dt 2 κ ) a + g σ 2 dσ =(i dt 2 γ 2 γ d) σ + g σ z a a(0) = 0,σ(0) = 1 σ z a = a c 1 = ( i 2 κ 2 ) c2 = ( i 2 γ 2 γ d) λ = c 1 +c 2 (c 1 c 2 ) 2 4g 2 λ + = c 1 +c 2 + (c 1 c 2 ) 2 4g 2 a(t) = (eλ +t e λ t )g (c1 c 2 ) 2 4g 2 σ(t) = (c 1 c 2 )(e λ t e λ +t )+ (c 1 c 2 ) 2 4g 2 (e λ t + e λ +t ) 2 (c 1 c 2 ) 2 4g 2
79 E (+) = γσê NV + κaê c + c.c., ê NV ê c ˆf( k, ω) E + = U F ( γσê NV + κaê c ), U F = k,ω ( ˆf( k, ω))( ˆf( k, ω) ) S(ω) 0 E + (t)e (t ) dtdt ω = ω c,κ γ d,g γ d,κ S (ω) ê NV U F ê NV +2R[ê NV U F ê c e i φ f c 1 ( r ) 1+i(ω ω c )/κ ]+ ê c U F ê c f c 1 ( r ) 1+i(ω ω c )/κ 2, F =(g( r, µ )) 2 /κγ r µ / µ ê NV U F ê c S d (ω) =C 1 +2C 2 R[e i φ f c 1 ( r ) 1+i(ω ω c )/κ ]+C 3f c 1 ( r ) 1+i(ω ω c )/κ 2,
80 C i C 2 /C C 2 /C 1 0 PL(ω, r) e( r ) PL(ω, r) = e( r r )S d (ω, r )dl dl r PL(ω, r) = S d (ω, r) e ( r ) PL ( r ) S d (ω, r ) e ( r )
81
82
83 9 F (τ) =A + Be (τ/t 2) n e ((τ jtrev)/t dec) 2, j=0 A =0.844 ± B =0.143 ± n =1.72 ± 0.14 T rev = ± 0.04µ T dec =7.47 ± 0.22µ T 2 = 201 ± 7µ 0 g 1 g 0 0 γ 1 γ 0 γ 1,0 0 τ 1 t 1 γ 1 (t R t 1 )+γ 0 t 1 t R p(n NV, odd) = tr 0 i 1 j=1 dτe (g 0 g 1 )τ g 0 t R (tr τ) (j 1) k=1 t k 0 i=1 g i 1g i 1 0 i 1 j=1 τ (j 1) k=1 τ k 0 ds j dt j PoissPDF(γ 1 τ + γ 0 (t R τ),n)
84 p(n NV, even) = tr 0 i 1 j=1 dτe (g 0 g 1 )τ g 0 t R (tr τ) (j 1) k=1 t k 0 i=1 (g 1 g 0 ) i i j=1 τ (j 1) k=1 τ k 0 dτ j dt j PoissPDF(γ 1 τ + γ 0 (t R τ),n) +e g 1t R PoissPDF(γ 1 t R,n) τ [0,t R ] PoissPDF(x, n) n x p(n NV, even) i p(n NV, odd) = p(n NV, even) = tr 0 tr 0 dτg 1 e (g 0 g 1 )τ g 0 t R BesselI(0, 2 g 1 g 0 τ(t R τ)) g1 g 0 τ dτ t R τ e(g 0 g 1 )τ g 0 t R BesselI(1, 2 g 1 g 0 τ(t R τ)) +e g 1t R PoissPDF(γ 1 t R,n), BesselI(n, x)
85 F C T 1/g 1 (P ) 594 P T T g 1 g 0,1 g 0 /g 1 = p(nv )/p(nv 0 ) a P/(1 + P/P sat )+dc P sat dc ap 2 /(1 + P/P sat ) P sat
86 594 g 0 ap 2 /(1 + P/P sat ) P sat = 134 a = 39 µ 2 g 1 ap 2 /(1 + P/P sat ) P sat = 53.2 a = 310 µ 2 γ 0 a P/(1 + P/P sat )+dc dc =0.268 a =1.65 µ P sat = 134 γ 1 a P/(1 + P/P sat )+dc a = 46.2 µ P sat = 53 γ 0,1 g 0,1
87 F C n thresh =[1, 2, 3] F C F C (P, t R ) n n thresh NV n<n thresh NV 0 t R n thresh =[1, 2, 3] m s =0 t I τ t R
88 N T = N(τ + t I + t R ) ( gµb Bτ ψ(τ) = cos π ) m s =0 i sin ( gµb Bτ π ) m s =1, g g B m s =0, m s =1 ( ) p 0 = cos 2 gµb Bτ π p 1 = 1 p 0 =sin 2 ( gµb Bτ π ). D 0 (n) D 1 (n) ψ(τ) P (n) =p 0 D 0 (n)+p 1 D 1 (n). δb S = n σ S δb = σ S S/ B = π gµ B τ σ S D 0 D 1,
89 p 0 = p 1 =1/2 N 1/ N σ R δb = π τ + ti + t R σ R 2gµ B T τ 2. = 2gµ Bτ π σ S S/ B σ R =1 σ R t I t R σ R σ R m s =0 m s =1 β 0 m s =0 β 1 m s =1 D 0 (n) D (n) 0 π 2gµ B =8.9 1
90 D D 0 σd 2 σ 2 D 0 P (n) =p 0 (β 0 D (n)+(1 β 0 )D 0 (n)) + (1 p 0 )(β 1 D (n)+(1 β 1 )D 0 (n)) σ R p 0 = p 1 =1/2 σr SCC = 2gµ Bτ σ S π S/ B S = p 0 (β 0 D +(1 β 0 ) D 0 )+(1 p 0 )(β 1 D +(1 β 1 ) D 0 ) = β ( 0 + β 1 D + 1 β ) 0 + β 1 D S B = gµ Bτ π (β 0 β 1 )( D D 0 ) [ ] σs 2 = n 2 P (n) S 2 σ SCC R = n=0 = 1 4 (β 0 + β 1 )(2 β 0 β 1 )( D D 0 ) 2 + β ( 0 + β 1 σd β ) 0 + β 1 σ 2 D (β 0 + β 1 )(2 β 0 β 1 ) (β 0 β 1 ) σ2 D /(2 β 0 β 1 )+σ 2 D 0 /(β 0 + β 1 ) ( D D 0 ) 2
91 σ R D (n) D 0 (n) σ SCC R (β 0 + β 1 )(2 β 0 β 1 ) (β 0 β 1 ) 2. β 0 β 1 m s =0 m s =1 σ R β 0,1 m s =0 m s =1 β 0,1 σr SCC (t R ) σ SCC R t R t R σr SCC
92 σr SCC σr SCC (t R ) D D 0 D (n) σ D D γ 1 t R σ SCC R (β 0 + β 1 )(2 β 0 β 1 ) 2 (β 0 β 1 ) (2 β 0 β 1 )γ 1 t R γ 1 t 3/4 σ SCC R σ SCC R = a 1+b/t 1/4 a =1.328 b = 39.3 a σr,best SCC
93
94
95
96 ɛ
97
98
99
100
101
102
Determining the Elastic Modulus and Hardness of an Ultrathin Film on a Substrate Using Nanoindentation
Determining the Elastic Modulus and Hardness of an Ultrathin Film on a Substrate Using Nanoindentation The Harvard community has made this article openly available. Please share how this access benefits
Φ / Resonant frequency (GHz) exp. theory Supplementary Figure 2: Resonant frequency ω PO
1 a 1 mm b d SQUID JJ c 30 µm 30 µm 10 µm Supplementary Figure 1: Images of the parametric phase-locked oscillator. a, Optical image of the device. The λ/4-type coplanar waveguide resonator is made of
arxiv: v1 [quant-ph] 1 Oct 2014
![arxiv: v1 [quant-ph] 1 Oct 2014](/thumbs/80/80458518.jpg "arxiv: v1 [quant-ph] 1 Oct 2014")
Efficient readout of a single spin state in diamond via spin-to-charge conversion arxiv:141.37v1 [quant-ph] 1 Oct 214 B. J. Shields, 1 Q. P. Unterreithmeier, 1 N. P. de Leon, 1 H. Park, 2, 1 and M. D.
Open Quantum Systems and Markov Processes II
Open Quantum Systems and Markov Processes II Theory of Quantum Optics (QIC 895) Sascha Agne sascha.agne@uwaterloo.ca July 20, 2015 Outline 1 1. Introduction to open quantum systems and master equations
Voc impact of orientation-dependent x in anisotropic PV absorbers.
Voc impact of orientation-dependent x in anisotropic PV absorbers The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Chakraborty,
Software Contracts for Security
Software Contracts for Security The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Moore, Scott David. 2016. Software Contracts
2 Quantization of the Electromagnetic Field
2 Quantization of the Electromagnetic Field 2.1 Basics Starting point of the quantization of the electromagnetic field are Maxwell s equations in the vacuum (source free): where B = µ 0 H, D = ε 0 E, µ
Lecturer: Bengt E W Nilsson
2009 05 07 Lecturer: Bengt E W Nilsson From the previous lecture: Example 3 Figure 1. Some x µ s will have ND or DN boundary condition half integer mode expansions! Recall also: Half integer mode expansions
Exploiting pattern transformation to tune phononic band gaps in a two-dimensional granular crystal
Exploiting pattern transformation to tune phononic band gaps in a two-dimensional granular crystal The Harvard community has made this article openly available. Please share how this access benefits you.
Understanding Nanoplasmonics. Greg Sun University of Massachusetts Boston
Understanding Nanoplasmonics Greg Sun University of Massachusetts Boston Nanoplasmonics Space 100pm 1nm 10nm 100nm 1μm 10μm 100μm 1ns 100ps 10ps Photonics 1ps 100fs 10fs 1fs Time Surface Plasmons Surface
Particle Physics II CP violation. Lecture 3. N. Tuning. (also known as Physics of Anti-matter ) Niels Tuning (1)
Particle Physics II CP violation (also known as Physics of Anti-matter ) Lecture 3 N. Tuning Niels Tuning (1) Plan 1) Mon 5 Feb: Anti-matter + SM 2) Wed 7 Feb: CKM matrix + Unitarity Triangle 3) Mon 26
Synthesizing arbitrary photon states in a superconducting resonator
Synthesizing arbitrary photon states in a superconducting resonator Max Hofheinz, Haohua Wang, Markus Ansmann, R. Bialczak, E. Lucero, M. Neeley, A. O Connell, D. Sank, M. Weides, J. Wenner, J.M. Martinis,
Atominstitut, Vienna University of Technology, Stadionallee 2, 1020 Vienna, Austria
Protecting a spin ensemble against decoherence in the strong-coupling regime of cavity QED S. Putz, 1, 2 D. O. Krimer, 3 R. Amsüss, 1 A. Valookaran, 1 T. Nöbauer, 1 J. Schmiedmayer, 1 S. Rotter, 3 and
Directional Statistics by K. V. Mardia & P. E. Jupp Wiley, Chichester, Errata to 1st printing
Directional Statistics K V Mardia & P E Jupp Wiley, Chichester, 2000 Errata to 1st printing 8 4 Insert of after development 17 3 Replace θ 1 α,, θ 1 α θ 1 α,, θ n α 19 1 = (2314) Replace θ θ i 20 7 Replace
Whitney Grummon. She kick started a fire in my soul Teaching me a tool to cleanse my mind That ll last a life time. That s how I will remember
W Gmm S kk f m T m m m T f m T I mmb N m p f p f f G L A f b k, b k v M k b p:, bb m, m f m, v. A b m, f mm mm f v b G p. S m m z pp pv pm f, k mk, f v M. I m, I m, fm k p x. S f 45 m m CMS, I p mf,. B
Nonlinear Oscillators and Vacuum Squeezing
Nonlinear Oscillators and Vacuum Squeezing David Haviland Nanosturcture Physics, Dept. Applied Physics, KTH, Albanova Atom in a Cavity Consider only two levels of atom, with energy separation Atom drifts
Spin-Boson Model. A simple Open Quantum System. M. Miller F. Tschirsich. Quantum Mechanics on Macroscopic Scales Theory of Condensed Matter July 2012
Spin-Boson Model A simple Open Quantum System M. Miller F. Tschirsich Quantum Mechanics on Macroscopic Scales Theory of Condensed Matter July 2012 Outline 1 Bloch-Equations 2 Classical Dissipations 3 Spin-Boson
Quantization of the open string on exact plane waves and non-commutative wave fronts
Quantization of the open string on exact plane waves and non-commutative wave fronts F. Ruiz Ruiz (UCM Madrid) Miami 2007, December 13-18 arxiv:0711.2991 [hep-th], with G. Horcajada Motivation On-going
Quantum technologies based on nitrogen-vacancy centers in diamond: towards applications in (quantum) biology
Quantum technologies based on nitrogen-vacancy centers in diamond: towards applications in (quantum) biology 3 E 532 nm 1 2δω 1 Δ ESR 0 1 A 1 3 A 2 Microwaves 532 nm polarization Pulse sequence detection
Efficient light emission from LEDs, OLEDs, and nanolasers via surface-plasmon resonance
Efficient light emission from LEDs, OLEDs, and nanolasers via surface-plasmon resonance Seok Ho Song, Hanyang University, http://optics.anyang.ac.kr/~shsong silver grating Key notes 1. How does the surface
2017 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future media,
7 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future media, including reprinting/republishing this material for advertising
Last Lecture. Overview and Introduction. 1. Basic optics and spectroscopy. 2. Lasers. 3. Ultrafast lasers and nonlinear optics
Last Lecture Overview and Introduction 1. Basic optics and spectroscopy. Lasers 3. Ultrafast lasers and nonlinear optics 4. Time-resolved spectroscopy techniques Jigang Wang, Feb, 009 Today 1. Spectroscopy
Origin of Optical Enhancement by Metal Nanoparticles. Greg Sun University of Massachusetts Boston
Origin of Optical Enhancement by Metal Nanoparticles Greg Sun University of Massachusetts Boston Nanoplasmonics Space 100pm 1nm 10nm 100nm 1μm 10μm 100μm Photonics 1ns 100ps 10ps 1ps 100fs 10fs 1fs Time
PART 2: INTRODUCTION TO CONTINUUM MECHANICS
7 PART : INTRODUCTION TO CONTINUUM MECHANICS In the following sections we develop some applications of tensor calculus in the areas of dynamics, elasticity, fluids and electricity and magnetism. We begin
Strong-electric-field effects and antenna resonances in single-wall carbon nanotube films
Strong-electric-field effects and antenna resonances in single-wall carbon nanotube films Dalius Seliuta Center for Physical Sciences and Technology, Vilnius, Lithuania Liudas Subačius, Irmantas Kašalynas,
Theoretical Photochemistry WiSe 2016/17
Theoretical Photochemistry WiSe 2016/17 Lecture 8 Irene Burghardt burghardt@chemie.uni-frankfurt.de) http://www.theochem.uni-frankfurt.de/teaching/ Theoretical Photochemistry 1 Topics 1. Photophysical
Radiative heat transfer
Radiative heat transfer 22 mars 2017 Energy can be transported by the electromagnetic field radiated by an object at finite temperature. A very important example is the infrared radiation emitted towards
Colby College Catalogue
Colby College Digital Commons @ Colby Colby Catalogues College Archives: Colbiana Collection 1866 Colby College Catalogue 1866-1867 Colby College Follow this and additional works at: http://digitalcommons.colby.edu/catalogs
NTC Disc Thermistors ND 03/06/09 NE 03/06/09 NV 06/09 APPLICATIONS TECHNOLOGY PERFORMANCE CHARACTERISTICS OPTIONS STANDARDIZATION
ND 03/06/09 NE 03/06/09 NV 06/09 APPLICATIONS Commodity Product: 2 families ND or NE : general purpose NV : professional Alarm and temperature measurement application Temperature regulation application
Lecture 9: RR-sector and D-branes
Lecture 9: RR-sector and D-branes José D. Edelstein University of Santiago de Compostela STRING THEORY Santiago de Compostela, March 6, 2013 José D. Edelstein (USC) Lecture 9: RR-sector and D-branes 6-mar-2013
Abelian and non-abelian Hopfions in all odd dimensions
Abelian and non-abelian Hopfions in all odd dimensions Tigran Tchrakian Dublin Institute for Advanced Studies (DIAS) National University of Ireland Maynooth, Ireland 7 December, 2012 Table of contents
Supplementary information
Supplementary information April 16, 2008 Development of collective modes The atoms in our system are confined at many locations within a one dimensional optical lattice of wavevector k t /850 nm, yet interact
Optomechanically induced transparency of x-rays via optical control: Supplementary Information
Optomechanically induced transparency of x-rays via optical control: Supplementary Information Wen-Te Liao 1, and Adriana Pálffy 1 1 Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg,
Basics of Infrared Detection
2 Basics of Infrared Detection Before the in-depth analyses of quantum well, ISBT, and QWIP a specific infrared detector we first discuss the general concept of how the temperature of an object influences
SUPPLEMENTARY INFORMATION
In the format provided by the authors and unedited. NATURE PHYSICS www.nature.com/naturephysics 1 285 x 5 15 5 25 1 1 Ω/µ 3 x C c = 4 6.5 3 µ 2 ε r =7 1.4 9 11 2 1 54 12 1 2 4 12 2 12 µ 2 12 12 12 12 NATURE
Lecture 2 Solutions to the Transport Equation
Lecture 2 Solutions to the Transport Equation Equation along a ray I In general we can solve the static transfer equation along a ray in some particular direction. Since photons move in straight lines
R k. t + 1. n E t+1 = ( 1 χ E) W E t+1. c E t+1 = χ E Wt+1 E. Γ E t+1. ) R E t+1q t K t. W E t+1 = ( 1 Γ E t+1. Π t+1 = P t+1 /P t
R k E 1 χ E Wt E n E t+1 t t + 1 n E t+1 = ( 1 χ E) W E t+1 c E t+1 = χ E Wt+1 E t + 1 q t K t Rt+1 E 1 Γ E t+1 Π t+1 = P t+1 /P t W E t+1 = ( 1 Γ E t+1 ) R E t+1q t K t Π t+1 Γ E t+1 K t q t q t K t j
Photoelectric readout of electron spin qubits in diamond at room temperature
Photoelectric readout of electron spin qubits in diamond at room temperature. Bourgeois,, M. Gulka, J. Hruby, M. Nesladek, Institute for Materials Research (IMO), Hasselt University, Belgium IMOMC division,
t [0, ) N 2 S s > 0 R IR\0 h > 0 θ 0, 1 θ = 1 λ 1 > 0 θ = 0 λ 0 0 λ 0 < λ 1 θ t = 0,, 2,... > 0 S r 0 e r t s dt = (1 δ)s δ = e r r > 0 [ θ R ] E r 0 e r t h dn θ,t N θ,t λ θ N θ,t λ θ t 0 r e r t h λ
Appendix A Spin-Weighted Spherical Harmonic Function
Appendix A Spin-Weighted Spherical Harmonic Function Here, we review the properties of the spin-weighted spherical harmonic function. In the past, this was mainly applied to the analysis of the gravitational
University of New Mexico
Quantum State Reconstruction via Continuous Measurement Ivan H. Deutsch, Andrew Silberfarb University of New Mexico Poul Jessen, Greg Smith University of Arizona Information Physics Group http://info.phys.unm.edu
Nuclear spin maser with a novel masing mechanism and its application to the search for an atomic EDM in 129 Xe
Nuclear spin maser with a novel masing mechanism and its application to the search for an atomic EDM in 129 Xe A. Yoshimi RIKEN K. Asahi, S. Emori, M. Tsukui, RIKEN, Tokyo Institute of Technology Nuclear
C c V Det. V Emi. C Self R S,E
Z( ) ( ) S I,Em (A /Hz) S V,Det (V /Hz) SUPPLEMENTARY INFORMATION: DETECTING NOISE WITH SHOT NOISE USING ON-CHIP PHOTON DETECTOR SUPPLEMENTARY FIGURES (a) V Emi C c V Det S I,Emi R E S I,SE C Self R S,E
S. Blair February 15,
S Blair February 15, 2012 66 32 Laser Diodes A semiconductor laser diode is basically an LED structure with mirrors for optical feedback This feedback causes photons to retrace their path back through
Dynamic Asset Allocation - Identifying Regime Shifts in Financial Time Series to Build Robust Portfolios
Downloaded from orbit.dtu.dk on: Jan 22, 2019 Dynamic Asset Allocation - Identifying Regime Shifts in Financial Time Series to Build Robust Portfolios Nystrup, Peter Publication date: 2018 Document Version
Quantum Optics in Wavelength Scale Structures
Quantum Optics in Wavelength Scale Structures SFB Summer School Blaubeuren July 2012 J. G. Rarity University of Bristol john.rarity@bristol.ac.uk Confining light: periodic dielectric structures Photonic
Fluence dependent variations of recombination and deep level spectral characteristics in neutron and proton irradiated MCz, FZ and epi-si structures
Outline Fluence dependent variations of recombination and deep level spectral characteristics in neutron and proton irradiated MCz, FZ and epi-si structures Motivation of combined investigations: E.Gaubas,
Fabrication and Measurement of Spin Devices. Purdue Birck Presentation
Fabrication and Measurement of Spin Devices Zhihong Chen School of Electrical and Computer Engineering Birck Nanotechnology Center, Discovery Park Purdue University Purdue Birck Presentation zhchen@purdue.edu
Cooling Using the Stark Shift Gate
Imperial College London Cooling Using the Stark Shift Gate M.B. Plenio (Imperial) A. Retzker (Imperial) Maria Laach 7/3/007 Department of Physics and Institute for Mathematical Sciences Imperial College
Active Medium Acceleration
Active Medium Acceleration Levi Schächter Department of Electrical Engineering Technion - Israel Institute of Technology Haifa 3, ISRAEL Outline Acceleration concepts Wake in a medium Frank-Hertz, LASER
r(equivalent): A Simple Effect Size Indicator
r(equivalent): A Simple Effect Size Indicator The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Rosenthal, Robert, and
Exam 8N080 - Introduction to MRI
Exam 8N080 - Introduction to MRI Friday April 10 2015, 18.00-21.00 h For this exam you may use an ordinary calculator (not a graphical one). In total there are 5 assignments and a total of 50 points can
140a Final Exam, Fall 2007., κ T 1 V P. (? = P or V ), γ C P C V H = U + PV, F = U TS G = U + PV TS. T v. v 2 v 1. exp( 2πkT.
4a Final Exam, Fall 27 Data: P 5 Pa, R = 8.34 3 J/kmol K = N A k, N A = 6.2 26 particles/kilomole, T C = T K 273.5. du = TdS PdV + i µ i dn i, U = TS PV + i µ i N i Defs: 2 β ( ) V V T ( ) /dq C? dt P?
FORMULATION OF ANISOTROPIC MEDIUM IN SPATIAL NETWORK METHOD. N. Yoshida, S. Koike, N. Kukutsu, and T. Kashiwa
Progress In Electromagnetics Research, PIER 13, 293 362, 1996 FORMULATION OF ANISOTROPIC MEDIUM IN SPATIAL NETWORK METHOD N. Yoshida, S. Koike, N. Kukutsu, and T. Kashiwa 1. Introduction 2. Spatial Network
PART 2 : BALANCED HOMODYNE DETECTION
PART 2 : BALANCED HOMODYNE DETECTION Michael G. Raymer Oregon Center for Optics, University of Oregon raymer@uoregon.edu 1 of 31 OUTLINE PART 1 1. Noise Properties of Photodetectors 2. Quantization of
Laser processing of materials. Temperature distributions
Laser processing of materials Temperature distributions Prof. Dr. Frank Mücklich Dr. Andrés Lasagni Lehrstuhl für Funktionswerkstoffe Sommersemester 7 Contents: Temperature distributions 1. Definitions.
SUPPLEMENTARY FIGURES
1 SUPPLEMENTARY FIGURES Supplementary Figure 1: Schematic representation of the experimental set up. The PC of the hot line being biased, the temperature raises. The temperature is extracted from noise
Problem 1, Lorentz transformations of electric and magnetic
Problem 1, Lorentz transformations of electric and magnetic fields We have that where, F µν = F µ ν = L µ µ Lν ν F µν, 0 B 3 B 2 ie 1 B 3 0 B 1 ie 2 B 2 B 1 0 ie 3 ie 2 ie 2 ie 3 0. Note that we use the
Contribution of the Hanbury Brown Twiss experiment to the development of quantum optics
Contribution of the Hanbury Brown Twiss experiment to the development of quantum optics Kis Zsolt Kvantumoptikai és Kvantuminformatikai Osztály MTA Wigner Fizikai Kutatóközpont H-1121 Budapest, Konkoly-Thege
50%-50% Beam Splitters Using Transparent Substrates Coated by Single- or Double-Layer Quarter-Wave Thin Films
University of New Orleans ScholarWorks@UNO University of New Orleans Theses and Dissertations Dissertations and Theses 5-22-2006 50%-50% Beam Splitters Using Transparent Substrates Coated by Single- or
5 questions, 3 points each, 15 points total possible. 26 Fe Cu Ni Co Pd Ag Ru 101.
Physical Chemistry II Lab CHEM 4644 spring 2017 final exam KEY 5 questions, 3 points each, 15 points total possible h = 6.626 10-34 J s c = 3.00 10 8 m/s 1 GHz = 10 9 s -1. B= h 8π 2 I ν= 1 2 π k μ 6 P
4 4 N v b r t, 20 xpr n f th ll f th p p l t n p pr d. H ndr d nd th nd f t v L th n n f th pr v n f V ln, r dn nd l r thr n nt pr n, h r th ff r d nd
n r t d n 20 20 0 : 0 T P bl D n, l d t z d http:.h th tr t. r pd l 4 4 N v b r t, 20 xpr n f th ll f th p p l t n p pr d. H ndr d nd th nd f t v L th n n f th pr v n f V ln, r dn nd l r thr n nt pr n,
FOUNDATION STUDIES EXAMINATIONS June PHYSICS Semester One February Main
1 FOUNDATION STUDIES EXAMINATIONS June 2013 PHYSICS Semester One February Main Time allowed 2 hours for writing 10 minutes for reading This paper consists of 4 questions printed on 10 pages. PLEASE CHECK
Stability of local observables
Stability of local observables in closed and open quantum systems Angelo Lucia anlucia@ucm.es Universidad Complutense de Madrid NSF/CBMS Conference Quantum Spin Systems UAB, June 20, 2014 A. Lucia (UCM)
[variable] = units (or dimension) of variable.
![[variable] = units (or dimension) of variable.](/thumbs/95/122609291.jpg "[variable] = units (or dimension) of variable.")
Dimensional Analysis Zoe Wyatt wyatt.zoe@gmail.com with help from Emanuel Malek Understanding units usually makes physics much easier to understand. It also gives a good method of checking if an answer
Projection Filters. Chapter Filter projection in general
19 Chapter 2 Projection Filters Dynamics of open quantum systems take place in the space of density matrices, which can be a very high dimensional space, particularly when photon fields are involved. Strictly
ECE 305 Fall Final Exam (Exam 5) Wednesday, December 13, 2017
NAME: PUID: ECE 305 Fall 017 Final Exam (Exam 5) Wednesday, December 13, 017 This is a closed book exam. You may use a calculator and the formula sheet at the end of this exam. Following the ECE policy,
Nonlinear wave-wave interactions involving gravitational waves
Nonlinear wave-wave interactions involving gravitational waves ANDREAS KÄLLBERG Department of Physics, Umeå University, Umeå, Sweden Thessaloniki, 30/8-5/9 2004 p. 1/38 Outline Orthonormal frames. Thessaloniki,
Retract. Press down D RG MG LG S. Recess. I-V Converter VNA. Gate ADC. DC Bias. 20 mk. Amplifier. Attenuators. 0.
a Press down b Retract D RG S c d 2 µm Recess 2 µm.5 µm Supplementary Figure 1 CNT mechanical transfer (a) Schematics showing steps of pressing down and retracting during the transfer of the CNT from the
linear Colliders Sayipjamal Dulat, Kaoru Hagiwara and Yu Matsumoto Xinjiang University, China and KEK, Tsukuba, Japan
Measuring Triple Gauge Boson Couplings at e + e linear Colliders Sayipjamal Dulat, Kaoru Hagiwara and Yu Matsumoto Xinjiang University, China and KEK, Tsukuba, Japan Measuring Triple Gauge Boson Couplings
On the Perturbative Stability of des QFT s
On the Perturbative Stability of des QFT s D. Boyanovsky, R.H. arxiv:3.4648 PPCC Workshop, IGC PSU 22 Outline Is de Sitter space stable? Polyakov s views Some quantum Mechanics: The Wigner- Weisskopf Method
A study of some curvature operators near the Euclidian metric
A study of some curvature operators near the Euclidian metric Erwann Delay Univ. Avignon Jussieu, 28 mai 2014 A geometric operator Let κ, Λ R and let Ein(g) = Ric(g) + κr(g) g + Λ g S 2. Φ (Ein(g)) = Ein(Φ
Holographic Entanglement Entropy for Surface Operators and Defects
Holographic Entanglement Entropy for Surface Operators and Defects Michael Gutperle UCLA) UCSB, January 14th 016 Based on arxiv:1407.569, 1506.0005, 151.04953 with Simon Gentle and Chrysostomos Marasinou
Winter College on Optics and Energy February Photophysics for photovoltaics. G. Lanzani CNST of Milano Italy
13-4 Winter College on Optics and Energy 8-19 February 010 Photophysics for photovoltaics G. Lanzani CNST of IIT@POLIMI Milano Italy Winter College on Optics and Energy Guglielmo Lanzani CNST of IIT@POLIMI,
FOUNDATION STUDIES EXAMINATIONS June PHYSICS Semester One February Main
1 FOUNDATION STUDIES EXAMINATIONS June 2015 PHYSICS Semester One February Main Time allowed 2 hours for writing 10 minutes for reading This paper consists of 6 questions printed on 10 pages. PLEASE CHECK
Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca
Femtosecond laser microfabrication in polymers Prof. Dr. Cleber R. Mendonca laser microfabrication focus laser beam on material s surface laser microfabrication laser microfabrication laser microfabrication
828.^ 2 F r, Br n, nd t h. n, v n lth h th n l nd h d n r d t n v l l n th f v r x t p th l ft. n ll n n n f lt ll th t p n nt r f d pp nt nt nd, th t
2Â F b. Th h ph rd l nd r. l X. TH H PH RD L ND R. L X. F r, Br n, nd t h. B th ttr h ph rd. n th l f p t r l l nd, t t d t, n n t n, nt r rl r th n th n r l t f th f th th r l, nd d r b t t f nn r r pr
Ver Chap Lecture 15- ECE 240a. Q-Switching. Mode Locking. ECE 240a Lasers - Fall 2017 Lecture Q-Switch Discussion
ing Ver Chap. 9.3 Lasers - Fall 2017 Lecture 15 1 ing ing (Cavity Dumping) 1 Turn-off cavity - prevent lasing 2 Pump lots of energy into upper state - use pulsed pump 3 Turn cavity back on - all the energy
Relaxation of femtosecond photoexcited electrons in a polar indirect band-gap semiconductor nanoparticle
PRAMANA c Indian Academy of Sciences Vol. 64, No. 1 journal of January 25 physics pp. 111 118 Relaxation of femtosecond photoexcited electrons in a polar indirect band-gap semiconductor nanoparticle NAVINDER
Exact calculation for AB-phase effective potential via supersymmetric localization
Exact calculation for AB-phase effective potential via supersymmetric localization Exact calculation for AB-phase effective potential via supersymmetric localization Todayʼs concern is purely theoretical...
A Game-Theoretic Analysis of Games with a Purpose
A Game-Theoretic Analysis of Games with a Purpose The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters. Citation Published Version
Numerical Continuation and Normal Form Analysis of Limit Cycle Bifurcations without Computing Poincaré Maps
Numerical Continuation and Normal Form Analysis of Limit Cycle Bifurcations without Computing Poincaré Maps Yuri A. Kuznetsov joint work with W. Govaerts, A. Dhooge(Gent), and E. Doedel (Montreal) LCBIF
A2 Assignment zeta Cover Sheet. C3 Differentiation all methods. C3 Sketch and find range. C3 Integration by inspection. C3 Rcos(x-a) max and min
A Assignment zeta Cover Sheet Name: Question Done Backpack Ready? Topic Comment Drill Consolidation M1 Prac Ch all Aa Ab Ac Ad Ae Af Ag Ah Ba C3 Modulus function Bb C3 Modulus function Bc C3 Modulus function
Electron spins in nonmagnetic semiconductors
Electron spins in nonmagnetic semiconductors Yuichiro K. Kato Institute of Engineering Innovation, The University of Tokyo Physics of non-interacting spins Optical spin injection and detection Spin manipulation
what happens if we make materials smaller?
what happens if we make materials smaller? IAP VI/10 ummer chool 2007 Couvin Prof. ns outline Introduction making materials smaller? ynthesis how do you make nanomaterials? Properties why would you make
Supplementary Figure 1 XRD pattern of a defective TiO 2 thin film deposited on an FTO/glass substrate, along with an XRD pattern of bare FTO/glass
Supplementary Figure 1 XRD pattern of a defective TiO 2 thin film deposited on an FTO/glass substrate, along with an XRD pattern of bare FTO/glass and a reference pattern of anatase TiO 2 (JSPDS No.: 21-1272).
single-layer transition metal dichalcogenides MC2
single-layer transition metal dichalcogenides MC2 Period 1 1 H 18 He 2 Group 1 2 Li Be Group 13 14 15 16 17 18 B C N O F Ne 3 4 Na K Mg Ca Group 3 4 5 6 7 8 9 10 11 12 Sc Ti V Cr Mn Fe Co Ni Cu Zn Al Ga
Colby College Catalogue
Colby College Digital Commons @ Colby Colby Catalogues College Archives: Colbiana Collection 1871 Colby College Catalogue 1871-1872 Colby College Follow this and additional works at: http://digitalcommonscolbyedu/catalogs
Photon Storage in Lambda-type Optically Dense Atomic Media. IV. Optimal Control Using Gradient Ascent
Photon Storage in Lambda-type Optically Dense Atomic Media. IV. Optimal Control Using Gradient Ascent The Harvard community has made this article openly available. Please share how this access benefits
Surface Chemistry of Copper Precursors in Connection with Atomic Layer Deposition (ALD) Processes
Surface hemistry of opper Precursors in onnection with Atomic Layer Deposition (ALD) Processes The Harvard community has made this article openly available. Please share how this access benefits you. Your
EE 6313 Homework Assignments
EE 6313 Homework Assignments 1. Homework I: Chapter 1: 1.2, 1.5, 1.7, 1.10, 1.12 [Lattice constant only] (Due Sept. 1, 2009). 2. Homework II: Chapter 1, 2: 1.17, 2.1 (a, c) (k = π/a at zone edge), 2.3
Phys 4061 Lecture Thirteen Photodetectors
Phys 4061 Lecture Thirteen Photodetectors Recall properties of indirect band gap materials that are used as photodetectors Photoelectric Effect in Semiconductors hν > Eg + χ χ is the electron affinity
8.821 F2008 Lecture 12: Boundary of AdS; Poincaré patch; wave equation in AdS
8.821 F2008 Lecture 12: Boundary of AdS; Poincaré patch; wave equation in AdS Lecturer: McGreevy Scribe: Francesco D Eramo October 16, 2008 Today: 1. the boundary of AdS 2. Poincaré patch 3. motivate boundary
ME 375 EXAM #1 Friday, March 13, 2015 SOLUTION
ME 375 EXAM #1 Friday, March 13, 2015 SOLUTION PROBLEM 1 A system is made up of a homogeneous disk (of mass m and outer radius R), particle A (of mass m) and particle B (of mass m). The disk is pinned
Quantum Light-Matter Interactions
Quantum Light-Matter Interactions QIC 895: Theory of Quantum Optics David Layden June 8, 2015 Outline Background Review Jaynes-Cummings Model Vacuum Rabi Oscillations, Collapse & Revival Spontaneous Emission
Twistor Strings, Gauge Theory and Gravity. Abou Zeid, Hull and Mason hep-th/
Twistor Strings, Gauge Theory and Gravity Abou Zeid, Hull and Mason hep-th/0606272 Amplitudes for YM, Gravity have elegant twistor space structure: Twistor Geometry Amplitudes for YM, Gravity have elegant
Quantum Many-Body Phenomena in Arrays of Coupled Cavities
Quantum Many-Body Phenomena in Arrays of Coupled Cavities Michael J. Hartmann Physik Department, Technische Universität München Cambridge-ITAP Workshop, Marmaris, September 2009 A Paradigm Many-Body Hamiltonian:
a few more introductory subjects : equilib. vs non-equil. ISM sources and sinks : matter replenishment, and exhaustion Galactic Energetics
Today : a few more introductory subjects : equilib. vs non-equil. ISM sources and sinks : matter replenishment, and exhaustion Galactic Energetics photo-ionization of HII assoc. w/ OB stars ionization
NMDA receptor dependent functions of hippocampal networks in spatial navigation and memory formation de Oliveira Cabral, H.
UvA-DARE (Digital Academic Repository) NMDA receptor dependent functions of hippocampal networks in spatial navigation and memory formation de Oliveira Cabral, H. Link to publication Citation for published
Advanced Vitreous State The Physical Properties of Glass
Advanced Vitreous State The Physical Properties of Glass Active Optical Properties of Glass Lecture 21: Nonlinear Optics in Glass-Applications Denise Krol Department of Applied Science University of California,