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Itinerant ferromagnetism in an atomic Fermi gas: Influence of ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitSimons09i.pdf24 Aug 2020: Such behavior is born out around quan-tum criticality in a variety of experimental solid-state sys-tems including ZrZn2 16,17, UGe2 18, MnSi 19–23,CoS2 24, YbRh2Si2 25, ... A. Lograsso, and S. M. Stishov, Phys. Rev. B 79, 100401R 2009.24 M. -
Multiparticle instability in a spin-imbalanced Fermi gas
www.tcm.phy.cam.ac.uk/~tmw38/Whitehead18.pdf8 Jan 2018: The effect of Pauli blocking has been carefully analyzed[22–24] for the product of two (N,N) = (1,1) instabilities,and found to give only a small correction to the ... B81, 174514 (2010). [23] W. V. Pogosov and M. Combescot, Physica C 471, 566 -
Lecture 19 Radiative transitions Radiative transitions: background…
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec19_compressed.pdf22 Nov 2009: Synopsis: Lectures 20-24. 15 Scattering theory. Elastic scattering; cross section; method of particle waves; Bornapproximation; scattering of identical particles. -
An Open Drug Discovery Competition: Experimental Validation of…
www.tcm.phy.cam.ac.uk/~gjc29/papers/Todd20.pdf26 Nov 2021: Each of the compounds gives rise to effects on the parasite’sinternal Na+ concentration and pH that are consistent with PfATP4 inhibition.20,21,24. -
Design of a nickel-base superalloy using a neural network ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitJonesStoneConduit17.pdf24 Aug 2020: Domains of steels withidentical properties. Mater. Manuf. Process., 24:5358, 2009. [9] W. ... Parallel Computing, 21:1, 1995. [24] A. Gelman, G.O. Roberts, and W.R. -
Tail-regression estimator for heavy-tailed distributions of known…
www.tcm.phy.cam.ac.uk/~gjc29/papers/LopezRiosConduit19.pdf24 Aug 2020: μ n 1]. (24). The parameters {cn} in Eq. (23) can be obtained by regressionof {A(m)}MRm=1 to Eq. ... 24) 0.00057545(25) 2 8.25 0.5328499(24) 0.00057545(24). -
Superfluidity at the BEC-BCS crossover in two-dimensional Fermi gases …
www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitConlonSimons08.pdf24 Aug 2020: 17 and 24.They found a stable FFLO phase only on the BCS side of theresonance. ... Rev. B 75,. 184526 2007.24 W. Zhang and L.-M. Duan, Phys. -
DiceLattice_Jussieu_2013
www.tcm.phy.cam.ac.uk/BIG/gm360/DiceLattice_Jussieu_2013_web.pdf30 Jul 2013: 0) (!/2,0) (0,0) (0,!/2) (0,!) (!/2,!) (!,!)("x,"y). 0.21. 0.22. 0.23. 0.24. -
Template for Electronic Submission to ACS Journals
www.tcm.phy.cam.ac.uk/~tmw38/IrwinLevellWhiteheadSegallConduit20.pdf2 Oct 2021: QSAR methods 20 including decision trees and random forests 21–23, radial basis functions 24,. ... B. 24. Figure 9. Comparison of the results on the independent test set for best of four QSAR methods. -
Experimental Evidence Suggestive of AnomalousConsciousness…
www.tcm.phy.cam.ac.uk/~bdj10/psi/delanoy/delanoy.pdf13 Aug 1998: This meta-analysis, conducted by Radin and Nelson [24], involves the largestparapsychological database to date, with 832 series, of which 597 were experimental series and235 control series. ... Comments on Bem and Honorton, Psych. Bulletin 115 (1994), -
Absence of diagonal force constants in cubic Coulomb crystals
www.tcm.phy.cam.ac.uk/~gjc29/papers/AndrewsConduit20.pdf23 Dec 2020: royalsocietypublishing.org/journal/rspa. ResearchCite this article: Andrews B, Conduit G. 2020Absence of diagonal force constants in cubicCoulomb crystals. Proc.R.Soc.A 476:20200518.https://doi.org/10.1098/rspa.2020.0518. Received: 1 July -
Special Report For reprint orders, please contact:…
www.tcm.phy.cam.ac.uk/~gjc29/papers/IrwinMahmoudWhiteheadConduitSegall20.pdf24 Aug 2020: NV, USA, 24 August 2008. 10. Abadi M, Barham P, Chen J et al. -
energy momentum handout.dvi
www.tcm.phy.cam.ac.uk/~jsb56/resources/energymomentumhandout.pdf24 Oct 2022: Exercise 24. Consider the journey of a link of chain through the through the fountain.Identify where in the fountain the link’s momentum changes. ... on the above axes. 24. 10 ROCKETS. 10 Rockets. Rockets work in a very simple way. -
Theoretical Physics II
www.tcm.phy.cam.ac.uk/~rjs269/TP2/TP2y2024.pdf22 Jan 2024: 1.23)The evolution operator is. U(t) =. U1(t) 0 t < t1U2(t t1)U1(t1) t1 t < t2 (1.24)where Ui(t) = eiHi t/h̄ and Hi =. p22m. ... This is Feynman’spath integral. 24. 2.2 The propagator. The path integral is a tool for calculating the propagator -
1 Prediction of In Vivo Pharmacokinetic Parameters and Time–Exposure…
www.tcm.phy.cam.ac.uk/~gjc29/papers/ObrezanovaGreene22.pdf15 Apr 2022: tissues, on 159 structurally varied types of drugs, food components, and industrial chemicals.24 In this. ... spanning a time period of 2 min to 24 h. 2.1.1. -
Lecture 19 Radiative transitions Radiative transitions: background…
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec19.pdf22 Nov 2009: Synopsis: Lectures 20-24. 15 Scattering theory. Elastic scattering; cross section; method of particle waves; Bornapproximation; scattering of identical particles. -
Photon Induced Decoherence of a TransmonSuperconducting Charge Qubit…
www.tcm.phy.cam.ac.uk/~mjh261/pdfs/masters.pdf26 Feb 2018: 24). We see that the term proportional to σ̂↠corresponds. to exiting both the qubit and the cavity. -
Imputation of Assay Bioactivity Data Using Deep Learning
www.tcm.phy.cam.ac.uk/~tmw38/WhiteheadIrwinHuntSegallConduit19.pdf30 Jul 2019: in the extrapolation of the training data.24,25 This isconceptually similar to the approach taken to uncertaintyestimation in ensemble models, although here the underlyingmodel is a deep neural network and ... 1. Introduction to Methodology and Encoding -
sustainable handout.dvi
www.tcm.phy.cam.ac.uk/~jsb56/resources/sustainablehandout.pdf24 Oct 2022: Put this intothe table at the start of the workbook. Exercise 24. -
Unveil the unseen: Exploit information hidden in noise
www.tcm.phy.cam.ac.uk/~gjc29/papers/ZviazhynskiConduit22.pdf23 May 2023: Furthermore, the uncertainty is useful foraccelerating materials discovery by guiding where newexperiments should be performed in the materials space[22–24], and also for the identification of outliers anderroneous entries in -
1 Structure–Mechanical Stability Relations of Metal-Organic…
www.tcm.phy.cam.ac.uk/~gjc29/papers/Moghadam19.pdf24 Aug 2020: 1. Structure–Mechanical Stability Relations of Metal-Organic Frameworks via Machine Learning. Peyman Z. Moghadama,,#, Sven M. J. Roggec,#, Aurelia Lib, Chun-Man Chowb, Jelle Wiemec, Noushin. Moharramid, Marta Aragones-Angladab, Gareth Conduite, -
Lecture 3: Tensor Product Ansatz Dr Gunnar MöllerCavendish…
www.tcm.phy.cam.ac.uk/BIG/gm360/NT/Numerical_Techniques_Lecture_3_Slides.pdf24 Feb 2014: 0. 5. 10. 15. 20. 25. 18 20 22 24 26 28 30 32 34 36 38. -
Imputation of Assay Bioactivity Data Using Deep Learning
www.tcm.phy.cam.ac.uk/~gjc29/papers/WhiteheadIrwinHuntSegallConduit19.pdf31 Mar 2023: in the extrapolation of the training data.24,25 This isconceptually similar to the approach taken to uncertaintyestimation in ensemble models, although here the underlyingmodel is a deep neural network and ... 1. Introduction to Methodology and Encoding -
Grain growth behaviour during near-γ’ solvus thermal exposures in ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/CollinsConduit13.pdf24 Aug 2020: 22, 23, 24]. Follow-ing the model for normal grain growth, given in Equations 3 &4, the velocity, v, and mobility, M, are described by the follow-ing expressions; v = 12 -
The Journal ofChemical Physics ARTICLE scitation.org/journal/jcp…
www.tcm.phy.cam.ac.uk/~gjc29/papers/LiuAndrewsConduit19.pdf22 Aug 2021: 24 containing no exact. ... Hartree, Math. Proc. Cambridge Philos. Soc. 24, 111–132 (1928).13J. C. Slater, Phys. -
PHYSICAL REVIEW A 93, 022706 (2016) Pseudopotentials for an ...
www.tcm.phy.cam.ac.uk/~tmw38/Whitehead16.pdf15 Feb 2016: Remarkably, even atmean-field level the nontilted (θ = 0) system with an isotropicpotential is predicted to display an inhomogeneous stripe phase[24,25] that is robust to the inclusion of perturbative -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec22-24_compressed.pdf27 Nov 2009: Lecture 24. Relativistic Quantum Mechanics:Solutions of the Dirac equation. Relativistic quantum mechanics: outline. ... non-examinable in this course. Synopsis: Lectures 20-24. 15 Scattering theory†Elastic and inelastic scattering; †method of -
PHYSICAL REVIEW A 83, 053625 (2011) Itinerant ferromagnetism in ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/vonKeyserlingkConduit11.pdf24 Aug 2020: 3Physics Department, Ben Gurion University, Beer Sheva 84105, Israel(Received 26 March 2011; published 24 May 2011). ... and thescattering length a = g/2πh̄2(1/m 1/m) O(g2) [24].Consistent with the Hartree-Fock scheme we employed tocalculate the grand -
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, -
Diffusion Monte Carlo study of a spin-imbalanced two-dimensional…
www.tcm.phy.cam.ac.uk/~gjc29/papers/FooConduit19.pdf24 Aug 2020: Nakazawa, and J. Wosnitza, Phys. Rev. Lett. 99,187002 (2007). [24] R. -
Quantum Order-by-Disorder in Strongly Correlated Metals Andrew G.…
www.tcm.phy.cam.ac.uk/~gjc29/papers/GreenConduitKruger17.pdf24 Aug 2020: dau damping propagates under renormalization to allterms in an expansion of the action[22, 24–27]. ... 4. 4.5. 5. 5.5. 6. |q(rlu)|. T(K. ). 0.2 0.21 0.22 0.23 0.24. -
Phase Transitions and Collective Phenomena
www.tcm.phy.cam.ac.uk/~achc2/phase/notes.pdf4 Jan 2023: Phase Transitions and CollectivePhenomena. Anson Cheungachc2@cam.ac.uk. January 2023. ii. Preface. The fundamental goal of statistical mechanics is to provide a framework in which themicroscopic probabilistic description of systems with large -
Multiparticle instability in a spin-imbalanced Fermi gas
www.tcm.phy.cam.ac.uk/~gjc29/papers/WhiteheadConduit18i.pdf24 Aug 2020: The effect of Pauli blocking has been carefully analyzed[22–24] for the product of two (N,N) = (1,1) instabilities,and found to give only a small correction to the ... B81, 174514 (2010). [23] W. V. Pogosov and M. Combescot, Physica C 471, 566 -
PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/Whitehead16.pdf24 Aug 2020: Mueller, Phys. Rev. A 78,. 033607 (2008).[24] X. Li, J. Kolorenč, and L. -
jsbhandout.dvi
www.tcm.phy.cam.ac.uk/~jsb56/resources/specialrelativityhandout.pdf24 Oct 2022: 1. 1 v/c. (24). The above classical analysis is perfectly adequate for fire engines, but breaks down if the sourceis moving at a speed close to the speed of light. -
PHYSICAL REVIEW A 95, 013633 (2017) Effective-range dependence of ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/SchonenbergConduit17.pdf24 Aug 2020: We conclude thatin both cases there is no bound state and the potential istherefore completely characterized in terms of its scatteringphase shift [24]. ... 2. Pöschl-Teller. The Pöschl-Teller interaction gives the exact phase shiftwith scattering -
PHYSICAL REVIEW B 94, 035157 (2016) Jastrow correlation factor ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/WhiteheadMichaelConduit16.pdf24 Aug 2020: This system has beenwidely studied using QMC [24,29–31] and serves as an analogfor electrons in a conductor. ... Holzmann,. Phys. Rev. Lett. 97, 076404 (2006).[24] G. G. Spink, R. -
PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...
www.tcm.phy.cam.ac.uk/~tmw38/Whitehead16a.pdf5 Apr 2016: Mueller, Phys. Rev. A 78,. 033607 (2008).[24] X. Li, J. Kolorenč, and L. -
PHYSICAL REVIEW B 90, 184302 (2014) Extracting semiconductor band ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/MonserratConduitNeeds14.pdf24 Aug 2020: Giustino, Nat. Commun. 4, 2006 (2013).[24] P. Han and G. Bester, Phys. -
qcmft
www.tcm.phy.cam.ac.uk/~bds10/tp3/secqu.pdf10 Oct 2012: 24 CHAPTER 2. SECOND QUANTISATION. Our aim is to find an operator V̂ in second quantised form whose action on a many-bodystate gives. -
thesisforsending.dvi
www.tcm.phy.cam.ac.uk/~jsb56/resources/thesis.pdf24 Oct 2022: 23. 1.10 Stretching a nematic elastomer perpendicular to its di-rector 24. ... 21. hard and soft LCEs. value, giving. F = 12µ. (. λ21 λ22. λ23r. ). (1.24). This energy is minimized by λ3 = r1/3 and λ2 = λ1 = r. -
PHYSICAL REVIEW A 93, 022706 (2016) Pseudopotentials for an ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/WhiteheadConduit16.pdf24 Aug 2020: Remarkably, even atmean-field level the nontilted (θ = 0) system with an isotropicpotential is predicted to display an inhomogeneous stripe phase[24,25] that is robust to the inclusion of perturbative -
Exotic Non-Abelian Topological Defects in Lattice Fractional Quantum…
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.119.106801.pdf24 Sep 2017: More saliently, genons at ν 1 in our modelhave d 2 thus allowing for universal quantum compu-tation, while the quasiparticles of the MR state itself cannot[12,24]. ... E. Tai, M.Rispoli, R. Islam, and M. Greiner, Ultra-precise holographicbeam shaping -
Fragment Graphical Variational AutoEncoding for Screening Molecules…
www.tcm.phy.cam.ac.uk/~gjc29/papers/ArmitageConduitSirringhaus19.pdf24 Aug 2020: 24 X. Gao and Z. Zhao, Sci. China Chem., 2015, 58, 947–968. -
Density Waves and Supersolidity in Rapidly Rotating Atomic Fermi ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.99.190409.pdf12 Aug 2010: n 0 1 2 3 4 12cjg<0 0.726(4) 0.86(1) 0.91(1) 0.93(1) 0.95(1) 12cjg>0 1.556(4) 1.24(1) ... This (incompressible) filled LL will appear as astep in the transverse density profile, as measured in situ orin an expansion measurement [24]. -
FerroElectricHeatCap.tex
www.tcm.phy.cam.ac.uk/~gjc29/Thesis/Conduit.pdf24 Aug 2020: in the velocity distribution of an ultracold atomic gas [22–24], which is shown in. ... calculated. 24 CHAPTER 2. A MANY-FLAVOUR ELECTRON GAS. 2.1.1 Polarisability. In this section the MFEG polarisability is derived. -
Chapter 3 Operator methods inquantum mechanics While the wave ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_operator.pdf8 Oct 2009: 3.2. SYMMETRY IN QUANTUM MECHANICS 24. 3.2 Symmetry in quantum mechanics. -
Oscillating Systems Natural SciencesPhysics Part 1A J. S. Biggins ...
www.tcm.phy.cam.ac.uk/~jsb56/resources/oschandout.pdf24 Oct 2022: 7. 1. 0. 12. 0. 24. 02. 24. 0 1 2 3 4 5 6 7 8. ... 24. The vectorsum of thex1 andx2 phasors gives a third one representingx3, also spinning atω0. -
Paired Composite Fermion Phase of Quantum Hall Bilayers at ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.101.176803.pdf12 Aug 2010: 24 OCTOBER 2008. 0031-9007=08=101(17)=176803(4) 176803-1 2008 The American Physical Society. ... 24 OCTOBER 2008. 176803-2. CF-Fermi sea state is uniquely defined as filling two CFshells in each layer (at this flux, the pth CF shell has 2porbitals) [3,12] -
Predicting the Current and Future State of Batteries usingData-Driven …
www.tcm.phy.cam.ac.uk/~gjc29/papers/NgZhaoYanConduitSeh20.pdf24 Aug 2020: IEEE Trans. Energy Conver. 26, 1172–1180 (2011). 24. Sitterly, M., Wang, L.
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