Search
Search Funnelback University
11 -
30 of
3,383
search results for KA :ZA31
where 0
match all words and 3,383
match some words.
Results that match 1 of 2 words
-
PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/Whitehead16.pdf24 Aug 2020: 2), which gives. ψ cont0 (r) J0(kr) π. 2[γ ln(ka/2)] Y0(kr), (7). ... 9) of (kR)2/2π , and so describe the scattering correctto O((ka)4). -
PHYSICAL REVIEW A 96, 023619 (2017) Effective-range dependence of ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/SchonenbergVerpoortConduit17.pdf24 Aug 2020: cot[δ(k)] = 2π. ln(ka) k2R2eff. 4. (1). Here a is the scattering length and Reff the effective range. ... f (k) = 4 2. πln(ka) k2R2eff4 i. (8). Matching both expressions, we can express ω0 and λ in termsof a and Reff ,. ω0 = 8π R2eff. ln(qa), (9a). -
Machine learning to predict mesenchymal stem cell efficacy for…
www.tcm.phy.cam.ac.uk/~gjc29/papers/LiuLuOhConduit20.pdf11 Nov 2020: RESEARCH ARTICLE. Machine learning to predict mesenchymal. stem cell efficacy for cartilage repair. Yu Yang Fredrik LiuID1, Yin Lu2, Steve Oh2, Gareth J. ConduitID1. 1 Theory of Condensed Matter Group, Cavendish Laboratory, University of Cambridge, -
Quantum Order-by-Disorder in Strongly Correlated Metals Andrew G.…
www.tcm.phy.cam.ac.uk/~gjc29/papers/GreenConduitKruger17.pdf24 Aug 2020: Quantum Order-by-Disorder in Strongly Correlated Metals. Andrew G. Green,1 Gareth Conduit,2 and Frank Krüger1, 31London Centre for Nanotechnology, University College London,. Gordon St., London, WC1H 0AH, United Kingdom2TCM, Cavendish Laboratory, -
PHYSICAL REVIEW A 90, 033626 (2014) High-fidelity pseudopotentials…
www.tcm.phy.cam.ac.uk/~gjc29/papers/BugnionLopezRiosNeedsConduit14.pdf24 Aug 2020: δcont (k) ={. arctan(ka), = 0,0, > 0,. is the scattering phase shift in the angular momentum channel. ... RcontE,=0(r) =sin[kr δ0(k)]. kr,. where δ0(k) = arctan(ka) and k =. E. The continuityequations at the cutoff are. p(rc) = ln{. sin[krc δ0(k)]rc. -
Absence of diagonal force constants in cubic Coulomb crystals
www.tcm.phy.cam.ac.uk/~gjc29/papers/AndrewsConduit20.pdf23 Dec 2020: Math. Mech. Solids 13, 199–220. (doi:10.1177/. 1081286507086898)3. Grimvall G, Magyari-Köpe B, Ozoliņš V, Persson KA. -
NATURAL SCIENCES TRIPOS Part II Wednesday 13 January 2016 ...
www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam16sol.pdf20 Jan 2016: 2mṙθ̇ mrθ̈ = ka sin(θ θB). d. dt. L. ṙ=L. ... r= mr̈ = mrθ̇2 kr ka cos(θ θB). d. dt. L. -
qcmft
www.tcm.phy.cam.ac.uk/~bds10/tp3/secqu.pdf10 Oct 2012: Ĥ = JN S2 B.Z.Xk! ka†kak O(S0) (2.16). where! k = 2JS(1 cos k) = 4JS sin2(k/2) represents the dispersion relation of the spinexcitations. -
qcmft
www.tcm.phy.cam.ac.uk/~bds10/tp3/ps2.pdf10 Oct 2012: cos ka. ——————————————–. Quantum Condensed Matter Field Theory. -
Lecture I 1 Lecture I: Collective Excitations: From Particles ...
www.tcm.phy.cam.ac.uk/~bds10/tp3/lectures.pdf10 Nov 2013: ka†k. )] O(N. 1/20 ). cf. quantum AF in spin-wave approximation. ... 2. (akak a. †ka†k. )]As with quantum AF, Ĥ diagonalised by Bogoluibov transformation:(. -
phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/topol.pdf4 Apr 2010: The first indication of unusual behaviour in the two-dimensional XY -model (n = 2)appeared in an analysis of the high temperature series expansion by Stanley and Ka-plan (1971). -
16.4. PROBLEM SET IV 216 16.4 Problem Set IV ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/ps4.pdf22 Nov 2009: and verify that the scattering is isotropic when the energy of the incidentparticle or the size of the scatterer is sufficiently low, so that Ka 1.Obtain an expression for the -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec2_compressed.pdf21 Oct 2009: κa =. {ka tan(ka) evenka cot(ka) odd. κa =. (2ma2V0! 2 (ka)2. ... leads to the condition,. k [An1 cos(ka) Bn1 sin(ka) An] =2maV0! -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec2.pdf12 Oct 2009: κa =. {ka tan(ka) evenka cot(ka) odd. κa =. (2ma2V0! 2 (ka)2. ... leads to the condition,. k [An1 cos(ka) Bn1 sin(ka) An] =2maV0! -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec16-17_compressed.pdf17 Nov 2009: eikna = ks (eika eika). 1N. eikna2ks cos(ka). We therefore find that. ... Classical chain: normal modes. ωk = 2. ksm| sin(ka/2)|. At low energies, k 0, (i.e. -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec16-17.pdf17 Nov 2009: Substituted into the equations of motion, we obtain. (mω2 2ks ) = 2ks cos(ka). ... ksm| sin(ka/2)|. Classical chain: normal modes. ωk = 2. ksm| sin(ka/2)|. -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec15_compressed.pdf9 Nov 2009: For N lattice sites and periodic boundary condition, αnN = αn,solution given by αn =. 1N. eikna,. E = Ek =ε 2t cos(ka)1 S cos(ka). i.e. -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec15.pdf9 Nov 2009: For N lattice sites and periodic boundary condition, αnN = αn,solution given by αn =. 1N. eikna,. E = Ek =ε 2t cos(ka)1 S cos(ka). i.e. -
Chapter 10 From molecules to solids In the previous ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_molecular.pdf9 Nov 2009: Substitution confirms that this is a solution with energies(exercise),. Ek =ε 2t cos(ka)1 S cos(ka). -
Chapter 2 Quantum mechanics in onedimension Following the rules ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_1d.pdf8 Oct 2009: Thefigure (right) compares κa = ( 2mV0a. 2! 2 (ka)2)1/2 with ka tan(ka) for the even. ... Bn1 =2maV0! 2k Bn sin(ka) Bn cos(ka) An sin(ka). Advanced Quantum Physics.
Refine your results
Date
- 1,286 Past year
- 1,187 Past 6 months
- 1,179 2024
- 957 Past 3 months
- 915 Past month
- 909 Past fortnight
- 905 Past week
- 584 Uncertain
- 393 Today
- 320 Yesterday
- 163 2023
- 152 2022
- 144 2019
- 125 2018
- 105 2005
- 86 2013
- 83 2010
- 81 2014
- 76 2011
- 75 2017
- 71 2016
- 71 2021
- 69 2020
- 56 2015
- 54 2008
- 53 2012
- 42 2009
- 32 2007
- 29 2006
- 17 2004
- 11 2002
- 10 2001
- 9 2003
- 4 2000
- 1 1998
- 1 1999
Search history
Recently clicked results
Recently clicked results
Your click history is empty.
Recent searches
- Economics |u:www.cisl.cam.ac.uk (37) · moments ago
- tj KaKaotalk:PC53 |u:www2.mrc-lmb.cam.ac.uk (1) · moments ago
- `Faculty Board of Economics` (95) · moments ago
- ������������������katalk:za33���24������ ������������������������������������������������������������ (1) · moments ago
- Economics middle test |u:www.murrayedwards.cam.ac.uk (1,043) · moments ago
- �����������������������������katalk:za31���24������ ������������ ������ ������ ������������������������������������������/������/������������/���������/���������������/������ (2,114) · moments ago
- `School of Economics` (160) · moments ago
- `School of Economics` (69) · moments ago
- ������tj ������������KaKaotalk:PC53��������� ������������������ (47) · moments ago
- ���������������������KA���:PC53��� (584) · moments ago
- ���������������������KA���:ZA31���������������������,������������������,������������,������������,������op (1) · moments ago
- civil engineering tunnelling courses (1,462) · moments ago
- Economics Syllabus (4) · moments ago
- katalk:za31 24 / / / / / |u:www.corporateleadersgroup.com (199) · moments ago
- Economics (2,241) · moments ago
- `Watson A.A` (72) · moments ago
- `School of Economics` (104) · moments ago
- Economics National Final Examination |u:www.fitz.cam.ac.uk (1) · moments ago
- Economics middle test (35) · moments ago
- download |u:myheplus.com (2) · moments ago
Recent searches
Your search history is empty.