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  1. Results that match 1 of 2 words

  2. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/HPCAutumnAcademyTalk2022.pdf
    15 Sep 2022: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.

  3. Perspectives on itinerant ferromagnetism in an atomic Fermi gas ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MITTalk2010.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  4. Tale-46.dvi

    www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-46.pdf
    18 Oct 2003: "#$ %&')( ,. -/.1024365"798:;24<>=,:?8@7A0"7CBEDF?84GIHJ.184KL795NMPOQ3R5"790PBS3RT9:1UV8@7924362 BW?8S2? HX=03YBUZ7[0"?BW]:105_.1H8@792@3R2 BW:10TC7a b[c&de],:fBg362LBS]"7h8@792@3R2 ... 34n '51 1. ,3n4. mFÀTC.)24 TC.)2nÀT9.)2ÀÇT9.)2. n)b orm)m[t. :.

  5. Tale-09.dvi

    www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-09.pdf
    29 Sep 2004: Therefore, two hermitian opera-tors âx;y = Ax;yp2Hare well dened. As a result the ommutation relations ould be rewritten as[ax;ay = iL (24)[L;ax = iay (25)[L;ay = ... Indeed, we see that the ommutationrelations in the form of Eqs (24,25,26) forms the su

  6. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/GrapheneCentreTalk2022.pdf
    13 May 2022: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.

  7. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMCurrentResearchTalk2021.pdf
    10 Jan 2021: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.

  8. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ACSForceConstantsTalk2018.pdf
    24 Aug 2020: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27.

  9. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/A_STAR_Talkii2019.pdf
    10 Sep 2021: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.

  10. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMCurrentResearchTalk2022.pdf
    14 Mar 2022: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.

  11. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TowlerTalk2013.pdf
    24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.

  12. Modelling the magnetoresistance of disordered superconducting films…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/RoyalHollowayTalk2012.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  13. assessment of cold fusion research

    www.tcm.phy.cam.ac.uk/~bdj10/papers/storms/review8.html
    11 May 2002: Yun et al. [19]. 1991. Seebeck(e). Open and closed. 0.01. 0.24, 500. ... Flow-type(d). closed. 0.1. 1.2, 440. Ota et al. [24]. 1992. Flow-type.

  14. Theoretical Physics 1Answers to Examination 2002 Warning — these ...

    www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam02sol.pdf
    24 Jan 2002: f̃(ω) =. dt f(t)eiωt ; f(t) =1. 2π. dω f̃(ω)eiωt (24). ... G(x,t) = dωdk. (2π2). ei(kxωt). ρω2 iγω Tk2(29). A. (24 January 2002) (TURN OVER.

  15. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CambridgePhenomenonProgramTalk2021.pdf
    7 Nov 2021: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.

  16. Pseudopotentials reach for the stars Gareth Conduit TCM Group, ...

    www.tcm.phy.cam.ac.uk/events/esdg/2014/Conduit_Jan_2014.pdf
    8 Jan 2016: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.

  17. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/LuxembourgSpinOrbitMaterialsTalk2017.pdf
    24 Aug 2020: Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. Slide 28.

  18. Developments and applications of the OPTIMADE API for materials…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/OPTIMADE24.pdf
    24 Jun 2024: Dow. nloa. ded. on 6. /24/. 2024. 9:0. 7:32. AM. T. ... pril. 2024. Dow. nloa. ded. on 6. /24/. 2024. 9:0. 7:32.

  19. Gareth Conduit (Cavendish Laboratory) Quantum critical itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/StAndrewsTalk2008.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  20. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMCurrentResearch_2Talk2021.pdf
    14 Jun 2021: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.

  21. Tale-10.dvi

    www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-10.pdf
    5 Mar 2004: illation, isg() = g(; S1) = vuut 14Æ1T exp 24( Æ1)24Æ1T 35 : (21)5. ... 0: (24)We an redu e its order to get the equationT dfd f = J: (25)6.

  22. Advanced Quantum Physics Lecture Handout i Preface Quantum mechanics…

    www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_preface.pdf
    8 Oct 2009: subject. Although 24 lectures is a long course to prepare(!), it is still insufficientto cover all of the topics that different physicists will describe as “core”. ... 22-24 Relativistic quantum mechanics: History; Klein-Gordon equation;Dirac equation

  23. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/A_STAR_Talki2019.pdf
    10 Sep 2021: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.

  24. Pseudopotentials for a dipolarultracold atomic gas Thomas…

    www.tcm.phy.cam.ac.uk/events/esdg/2015/Whitehead_March_2015.pdf
    2 Jun 2016: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27.

  25. 20.7 News 230-231 MH

    www.tcm.phy.cam.ac.uk/~bdj10/articles/Reich_20Jul2006.pdf
    5 Sep 2006: 24% was how much global wind-power capacity increased last year. 80% of the world’s energy wasderived from fossil fuels in 2005.

  26. ��������� �� �������������������������� � �!��� �"…

    www.tcm.phy.cam.ac.uk/~nrc25/TP1/ExamFiles/exam00sol.pdf
    7 Jan 2019: " $#&%'() ,---./10 243 24567 849 : 9/24: ;<9 0 :=84/ >9?@9 9 2A BCD4E 9 7 9 E FG0 9 7 FHD@9 I@J J J KLE 9 /: 90

  27. Theoretical Physics 1Answers to Examination 2003 Warning — these ...

    www.tcm.phy.cam.ac.uk/~nrc25/TP1/ExamFiles/exam03sol.pdf
    7 Jan 2019: 2γ(tt′) sin (t t′). (24). We use the Green function to solve for the response to source f(t) by calculating.

  28. RAPID COMMUNICATIONS PHYSICAL REVIEW A 87, 060502(R) (2013)…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bugnion13ii.pdf
    24 Aug 2020: and three-body models [23,24,46,47], and losses tostates excited with transverse COM motion [13–15,25]. ... 103, 207201 (2009).[23] D. Pekker et al., Phys. Rev. Lett. 106, 050402 (2011).[24] C.

  29. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMCurrentResearchTalk2019.pdf
    24 Aug 2020: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.

  30. Tale 6 The Kramers’ Phase and Laplace’s Method The ...

    www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-06.pdf
    11 Sep 2010: y′′ x2y = λy (24). The asymptote of its solution at |x| is. ... x2. 2. ). (26). into Eq (24) leads to the following equation for Hλ(x) :. {. d2. dx2+ 2x. d. dx λ 1. }. Hλ(x) = 0 (27).

  31. Inhomogeneous Phase Formation on the Border of Itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitGreenSimons09.pdf
    24 Aug 2020: As a consequence, the coefficientof m4? in a Ginzburg-Landau expansion is proportional tothat of q2m2?: i.e., F ð þ k2Fq2=24 2a2Þm2? ... Tofurther optimize the wave function, the Slater determinantorbitals were evaluated at quasiparticle positions

  32. NATURAL SCIENCES TRIPOS Part II Wednesday 13 January 2010 ...

    www.tcm.phy.cam.ac.uk/~nrc25/TP1/ExamFiles/exam10sol.pdf
    7 Jan 2019: g. aB , ω2B = 12ga. l2(AB). so. ω2B = 12gal2B 24. ... 11. g2. l2ω2B ,. ω4 12gal2ω2 24. 11. g2. l2= 0 ,. and therefore. ω2 = 6ga. l2. 1. 1 2. 33. l2.

  33. Tale-45.dvi

    www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-45.pdf
    2 Jan 2007: z =x iy. 2, z̄ =. x iy2. , (24). =12. (.

  34. Le3.dvi

    www.tcm.phy.cam.ac.uk/~dek12/courses/phase/Le3.pdf
    29 Sep 2016: 24). The right-hand side of Eq (24) shows, in particular, thatthe total magnetic flux, associated with the single vortex,. ... 2The second part of Eq(24) can be obtained by integrating both its sides over asmall area near origin.

  35. examples_all.dvi

    www.tcm.phy.cam.ac.uk/~achc2/pt2thermo.pdf
    30 Apr 2011: KN =1. 4V. (. 2πh̄2. mekBT. )3/2. eeφ/kBT. where φ is the first ionisation potential of He, which is 24.6 V.Find the proportion of He that is ionised

  36. 1498390593355545040-09347118

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitConduitStoneHardy13.pdf
    30 Aug 2021: 45) Date of Patent: May 24, 2016. (54) ALLOY COMPOSITION (56) References Cited. ... U.S. Patent May 24, 2016 US 9,347,118 B2. 16OOP. 1400 - OptimalOW COstalloy'MoB.

  37. Itinerant ferromagnetism: A quantum fluctuation driven FFLO analogue…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/BirminghamTalk2009.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  38. Chapter 2 Ginzburg-Landau Phenomenology The divergence of the…

    www.tcm.phy.cam.ac.uk/~achc2/phase/GL.pdf
    25 Jan 2021: dCddx. =1. xd1Sd, Cd(x) =. x2d. (2d)Sd+ const., (2.19). 24 CHAPTER 2. ... Eq. (2.24) implies that preciselyat Tc, the correlations decay as 1/|x|d2.

  39. ANSWERS2004.dvi

    www.tcm.phy.cam.ac.uk/~nrc25/TP1/ExamFiles/exam04sol.pdf
    7 Jan 2019: 0. ux1du. 1 u= 2πi (24). Identifying the sin πx and dividing through, the required result is obtained.

  40. Microsoft PowerPoint - camlec9

    www.tcm.phy.cam.ac.uk/~amg73/cambmeso2012.pdf
    20 Jan 2017: . 22. AssesP. dD. Wigner Dyson statistics. 12 16 20 24 28 320.0. ... q. n. qLrdrψ. 12 16 20 24 28 320.0. 0.2. 0.4.

  41. Imputation of Sensory Properties Using DeepLearningMatthew Segall (  …

    www.tcm.phy.cam.ac.uk/~tmw38/Mahmoud21.pdf
    21 Nov 2022: 24] or Gaussian processes (GP) [25]. Sophisticated deep learning methods have also been applied to QSAR. ... 24] P. Hunt, L. Hosseini-Gerami, T. Chrien, J. Plante, D. Ponting and M.

  42. Inhomogeneous phase formation on the border of itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/WeizmannTalk2009.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  43. ��������� �� �������������������������� � �!��� �"…

    www.tcm.phy.cam.ac.uk/~nrc25/TP1/ExamFiles/exam01sol.pdf
    7 Jan 2019: " $#&%'() ,--. /10 243 24567 849 : 9/24: ;<9 0 :=84/ >9?@9 9 2A BCD4E 9 7 9 E FG0 9 7 FHD@9 I@J J J KLE 9 /: 90 ... kx m n l. q3 J 91JLz|{124IHP B0 I49 0 9 }u4/17 3 B124: v B10<7 849A BHB10 I43 24/17 9 : m n J 849bH3 249 7

  44. Theoretical Physics 1Answers to Examination 2005 Warning — these ...

    www.tcm.phy.cam.ac.uk/~nrc25/TP1/ExamFiles/exam05sol.pdf
    7 Jan 2019: z =1 p. 3i. 2+. q. 2. (1 p. 3i)2 4 q = 1 (24).

  45. Direct calculation of static response functions using non-diagonal…

    www.tcm.phy.cam.ac.uk/events/esdg/2015/LloydWilliams_June_2015.pdf
    2 Jun 2016: 4 8 12 16 20 24 28 32. Linear size of BZ grid. ... Thermal and optical band gaps of diamond. 4 8 12 16 20 24 28 32.

  46. March 5, 2021 8:54 IJAIT S0218213021500081 page 1 International ...

    www.tcm.phy.cam.ac.uk/~tmw38/Whitehead21.pdf
    2 Oct 2021: deep learning approaches,24 methods that mitigate against training time, as well. ... Ba, Adam: A method for stochastic optimization, arXiv e-prints,. art. arXiv:1412.6980 (2014).24.

  47. PHYSICAL REVIEW A 88, 013601 (2013) Exploring exchange mechanisms ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bugnion13i.pdf
    24 Aug 2020: and can be extended tolarger systems through a quantum virial or cluster expansion[24,25]. ... J. Phys. 79, 762 (2011).[24] X.-J. Liu, H. Hu, and P.

  48. Tale-03.dvi

    www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-03.pdf
    1 Aug 2004: Tale 3Supersymmetri Quantum Me hani s1. let us begin from well-known example of a linear os illator,whi h has the Hamiltonian:Ĥ = E ; Ĥ = p̂22m m!2x22 [p̂; x̂ = ih (1)Or, in dimensionless variables:P = vuut 1mh!p; q = sm!h x; (2)H = h! H; H =

  49. Dr Nicholas Hine I am a Winton Advanced Research ...

    www.tcm.phy.cam.ac.uk/~ndmh3/cv.pdf
    21 Feb 2013: Phys. Commun. 180, 1041 (2008). [24] N.D.M. Hine, W.M.C, Foulkes, Localization Lengths over Metal to Band Insulator transitions,J.

  50. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/A_STAR_Talk_2020.pdf
    11 Sep 2021: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.

  51. 16.1. PROBLEM SET I 197 Answers: Problem set I ...

    www.tcm.phy.cam.ac.uk/~bds10/aqp/ans1.pdf
    14 Oct 2009: quired identities. As a result, we can confirm that. [a, a†] =24.

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