{"id":17,"date":"2016-02-18T12:36:27","date_gmt":"2016-02-18T12:36:27","guid":{"rendered":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/?page_id=17"},"modified":"2022-10-31T14:30:01","modified_gmt":"2022-10-31T14:30:01","slug":"publications","status":"publish","type":"page","link":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/publications\/","title":{"rendered":"Publications"},"content":{"rendered":"

<\/a>[98] Ternary network models for disturbed ecosystems <\/strong> <\/b>
\nKieran Peel, Darren Evans and Clive Emary
\n<\/i>R. Soc. Open Sci. 9 220619 (2022) <\/a><\/p>\n

<\/a>[97] Network science: Applications for sustainable agroecosystems and food security<\/b>
\nFredric M. Windsor, et al.<\/i>
\nPerspectives in Ecology and Conservation (2022) <\/a><\/p>\n

<\/a>[96] Stability-instability transition in tripartite merged ecological networks<\/b>
\nClive Emary and Anne-Kathleen Malchow<\/i>
\nJ. Math. Bio. 85, 20 (2022) <\/a>, bioarXiv 2022.03.18.484866<\/a><\/p>\n

<\/a>[95] Quantum Computer Benchmarking via Quantum Algorithms<\/strong><\/b>
\nKonstantinos Georgopoulos, Clive Emary, and Paolo Zuliani<\/i>
\narXiv:2112.09457 <\/a><\/p>\n

<\/a>[94] Modeling and simulating the noisy behavior of near-term quantum computers <\/strong> <\/b>
\nKonstantinos Georgopoulos, Clive Emary, and Paolo Zuliani
\n<\/i>Phys. Rev. A 104, 062432 (2021)<\/a>, arXiv:2101.02109 <\/a><\/p>\n

<\/a>[93] Markets as ecological networks: inferring interactions and identifying communities <\/strong> <\/b>
\nClive Emary and Hugo Fort
\n<\/i>Journal of Complex Networks 9, cnab022 (2021) <\/a><\/p>\n

<\/a>[92] Can a complex ecosystem survive the loss of a large fraction of its species? A random matrix theory of secondary extinction <\/strong> <\/b>
\nClive Emary and Darren M Evans
\n<\/i>Oikos 130, 1512 (2021)<\/a><\/p>\n

<\/a>[91] Phase averaging and arrival times in a hot-electron Mach-Zehnder interferometer <\/strong><\/b>
\nClarissa J. Barratt, Sungguen Ryu, Lewis A. Clark, H. -S. Sim, Masaya Kataoka, and Clive Emary
\n<\/i> Phys. Rev. B 104, 035436 (2021)<\/a>, arXiv:2104.01653 <\/a><\/p>\n

<\/a>[90] Mitigating decoherence in hot electron interferometry <\/strong>
\nLewis A. Clark, Masaya Kataoka, and Clive Emary
\n<\/i> New J. Phys. 22 103031 (2020)<\/a>, arXiv:2003.06574 <\/a><\/b><\/p>\n

<\/a>[89] Comparison of quantum-walk implementations on noisy intermediate-scale quantum computers <\/strong><\/b>
\nKonstantinos Georgopoulos, Clive Emary, and Paolo Zuliani
\n<\/i> Phys. Rev. A 103, 022408 (2021)<\/a>, arXiv:1911.00305<\/a><\/p>\n

<\/a>[88] <\/b> Interplay of quantum phase transition and flat band in hybrid lattices <\/strong>
\nGui-Lei Zhu, Xin-You Lu, Hamidreza Ramezani, Clive Emary, Jin-Hua Gao, and Ying Wu
\n<\/i> Phys. Rev. Research 2, 033463 (2020)<\/a>, arXiv:1910.00747 <\/a><<\/p>\n

<\/a>[87] Counting statistics of dark-state transport through a carbon nanotube quantum dot <\/strong><\/b>
\nNathan Ho and Clive Emary
\n<\/i> Phys. Rev. B 100 245414 (2019)<\/a>, arXiv:1908.02026<\/a><\/p>\n

<\/a>[86] Experimental test of non-macrorealistic cat-states in the cloud <\/strong> <\/b>
\nHuan-Yu Ku, Neill Lambert, Fong-Ruei Jhan, Clive Emary, Yueh-Nan Chen, Franco Nori
\n<\/i> npj Quantum information 6, 98 (2020)<\/a>, arXiv:1905.13454<\/a><\/b><\/p>\n

<\/a>[85] Energy relaxation in hot electron quantum optics via acoustic and optical phonon emission <\/strong> <\/b>
\nC. Emary, L. A. Clark, M. Kataoka, N. Johnson
\n<\/i> Phys. Rev. B 99 045306 (2019)<\/a>, arXiv:1807.11814 <\/a><\/p>\n

<\/a>[84] Perpetual emulation threshold of PT-symmetric Hamiltonians <\/strong> <\/b>
\nD. Trypogeorgos, A. Vald\u00e9s-Curiel, I. B. Spielman, C. Emary
\n<\/i> J. Phys. A 51 325302 (2018)<\/a>, arXiv:1803.06548 <\/a><\/p>\n

<\/a>[83] LO-phonon emission rate of hot electrons from an on-demand single-electron source in a GaAs\/AlGaAs heterostructure <\/strong> <\/b>
\nN. Johnson, C. Emary, S. Ryu, H.-S. Sim, P. See, J. D. Fletcher, J. P. Griffiths, G. A. C. Jones, I. Farrer, D. A. Ritchie, M. Pepper, T. J. B. M. Janssen, M. Kataoka <\/i>
\nPhys. Rev. Lett. 121, 137703 (2018)<\/a>, arXiv:1712.09031<\/a><\/p>\n

<\/a>[82] Violations of a Leggett-Garg inequality without signalling for a photonic qutrit probed with ambiguous measurements<\/strong><\/b>
\nKunkun Wang, Clive Emary, Mengyan Xu, Xiang Zhan, Zhihao Bian, Lei Xiao, Peng Xue
\n<\/i> Phys. Rev. A 97 020101 (2018)<\/a>, arXiv:1711.05172<\/a><\/p>\n

<\/a>[81] Ambiguous measurements, signalling and violations of Leggett-Garg inequalities<\/strong> <\/b>
\nClive Emary
\n<\/i> Phys. Rev. A 96 042102 (2017)<\/a>, arXiv:1703.09547<\/a><\/p>\n

<\/a>[80] Coherent control in quantum transport: amplification, filtering and switching at finite bias<\/strong> <\/b>
\nRajpal Thethi, and Clive Emary
\n<\/i> Quantum Sci. Technol. 2, 024011 (2017)<\/a>, arXiv:1703.03672<\/a><\/p>\n

<\/a>[79] Enhanced violations of Leggett-Garg inequalities in an experimental three-level system <\/strong> <\/b>
\nKunkun Wang, Clive Emary, Xiang Zhan, Zhihao Bian, Jian Li, Peng Xue
\n<\/i> Optics Express 25, 31462 (2017)<\/a>, arXiv:1701.02454<\/a><\/p>\n

<\/a>[78] Atomic “bomb testing”: the Elitzur-Vaidman experiment violates the Leggett-Garg inequality<\/b>
\nCarsten Robens, Wolfgang Alt, Clive Emary, Dieter Meschede, and Andrea Alberti
\n<\/i>J. Apl. Phys. B 123, 12 (2016)<\/a>, arXiv:<\/a>1609.06218<\/a><\/p>\n

<\/a>[77] Feedback Control of Waiting Times <\/b>
\nTobias Brandes and Clive Emary
\n<\/i>Phys. Rev. E 93 042103 (2016),<\/a>arXiv:<\/a>1602.02975<\/a><\/p>\n

<\/a>[76] Time-of-Flight Measurements of Single-Electron Wave Packets in Quantum-Hall Edge States<\/b>
\nM. Kataoka, N. Johnson, C. Emary, P. See, J. P. Griffiths, G. A. C. Jones, I. Farrer, D. A. Ritchie, M. Pepper, and T. J. B. M. Janssen
\n<\/i> Phys. Rev. Lett. 116, 126803 (2016), <\/i><\/a>arXiv:1512.02906<\/a><\/p>\n

<\/a>[75] Phonon emission and arrival times of electrons from a single-electron source<\/b>
\nC. Emary, A. Dyson, Sungguen Ryu, H.-S. Sim, and M. Kataoka<\/i>
\nPhys. Rev. B 93, 035436 (2016)<\/a>, arXiv:1510.06922<\/a><\/p>\n

<\/a>[74] REVIEW: Feedback control in quantum transport<\/b>
\nClive Emary<\/i>
\nin Control of Self-Organizing Nonlinear Systems<\/a><\/em>, edited by E. Sch\u00f6ll, S. H. L. Klapp and P.
\nH\u00f6vel, (Springer 2016), arXiv:1507.05396<\/a><\/p>\n

<\/a>[73] Maximum violations of the quantum-witness equality<\/b>
\nGreg Schild and Clive Emary
\n<\/i>Phys. Rev. A 92, 032101 (2015)<\/a>, arXiv:1507.05328<\/a><\/p>\n

<\/a>[72] Testing macroscopic realism through high-mass interferometry<\/b>
\nClive Emary, J. P. Cotter, Markus Arndt
\n<\/i>Phys. Rev. A 90, 042114 (2014)<\/a>, arXiv:1408.1626<\/a><\/p>\n

<\/a>[71] On the waiting time distribution for continuous stochastic systems
\n<\/b>Robert Gernert, Clive Emary, Sabine H. L. Klapp
\n<\/i>Phys. Rev. E 90, 062115 (2014),  <\/a>arXiv:1407.1675<\/a><\/p>\n

<\/a>[70] Coherent feedback control in quantum transport<\/b>
\nClive Emary and John Gough<\/i>
\nPhys. Rev. B 90, 205436 (2014)<\/a>, arXiv:1407.1306<\/a><\/p>\n

<\/a>[69] Ideal Negative Measurements in Quantum Walks Disprove Theories Based on Classical Trajectories
\n<\/b>Carsten Robens, Wolfgang Alt, Dieter Meschede, Clive Emary, and Andrea Alberti
\n<\/i>Phys. Rev. X 5, 011003 (2015), <\/a>arXiv:1404.3912<\/a><\/p>\n

<\/a>[68] Time-delayed feedback control of the Dicke-Hepp-Lieb superradiant quantum phase transition
\n<\/b>Wassilij Kopylov, Clive Emary, Eckehard Sch\u00f6ll, and Tobias Brandes
\n<\/i>New J. Phys. 17, 013040 (2015), <\/a>arXiv:1403.0620<\/a><\/p>\n

<\/a>[67] Full counting statistics of random transition-rate matrices
\n<\/b>Uliana Mordovina and Clive Emary
\n<\/i>Phys. Rev. E 88, 062148 (2013), <\/a>arXiv:1310.4070<\/a><\/p>\n

<\/a>[66] Radical-pair model of magnetoreception with spin-orbit coupling
\n<\/b>Neill Lambert, Simone De Liberato, Clive Emary, and Franco Nori<\/i>
\nNew J. Phys. 15, 083024 (2013), <\/a>arXiv:1309.5882<\/a><\/p>\n

<\/a>[65] Temporal quantum correlations and Leggett-Garg inequalities in multi-level systems
\n<\/b>Costantino Budroni and Clive Emary
\n<\/i>Phys. Rev. Lett. 113, 050401 (2014)<\/a>, arXiv:1309.3678<\/a>
\n<\/a>[64] Non-equilibrium correlations and entanglement in a semiconductor hybrid circuit-QED system
\n<\/b>L. D. Contreras-Pulido, C. Emary, T. Brandes, R. Aguado
\n<\/i>New J. Phys. 15, 095008 (2013)<\/a>, arXiv:1304.7192<\/a><\/p>\n

<\/a>[63] Dark states in multi-mode multi-atom Jaynes-Cummings systems<\/b>
\nC. Emary
\n<\/i>J. Phys. B: At. Mol. Opt. Phys. 46, 224008 (2013)<\/a>, arXiv:1304.6240<\/a><\/p>\n

<\/a>[62] REVIEW ARTICLE: Leggett-Garg Inequalities
\n<\/b>C. Emary, N. Lambert, and F. Nori
\n<\/i>Rep. Prog. Phys. 77, 016001 (2014)<\/a>, arXiv:1302.5133<\/a><\/p>\n

<\/a>[61] Floquet Topological Quantum Phase Transitions in the transverse Wen-Plaquette Model<\/b>
\nV. M. Bastidas, C. Emary, G. Schaller, A. G\u00f3mez-Le\u00f3n, G. Platero, T. Brandes
\n<\/i>arXiv:1302.0781<\/a><\/p>\n

<\/a>[60] Counting statistics of the Dicke superradiance phase transition<\/b>
\nWassilij Kopylov, Clive Emary, Tobias Brandes<\/i>
\nPhys. Rev. A 87, 043840 (2013)<\/a>, arXiv:1301.2973<\/a><\/p>\n

<\/a>[59] Decoherence and maximal violations of the Leggett-Garg inequality
\n<\/b>C. Emary<\/i>
\nPhys. Rev. A 87, 032106 (2013)<\/a>, arXiv:1212.3865<\/a><\/p>\n

<\/a>[58] AC-driven Quantum Phase Transition in the Lipkin-Meshkov-Glick Model
\n<\/b>G. Engelhardt, V. M. Bastidas, C. Emary, T. Brandes
\n<\/i>Phys. Rev. E 87, 052110 (2013)<\/a>, arXiv:1211.2683<\/a><\/p>\n

<\/a>[57] Superradiant phase transition in a model of three-level-lambda systems interacting with two bosonic modes<\/b>
\nMathias Hayn, Clive Emary, Tobias Brandes<\/i>
\nPhys. Rev. A 86, 063822 (2012)<\/a>, arXiv:1209.3121<\/a><\/p>\n

<\/a>[56] The Leggett-Garg inequality in electron interferometers
\n<\/b>Clive Emary, Neill Lambert, Franco Nori<\/i>
\nPhys. Rev. B 86, 235447 (2012)<\/a>, arXiv:1209.2977<\/a><\/p>\n

<\/a>[55] A minimal model for short-time diffusion in periodic potentials<\/b>
\nClive Emary, Robert Gernert, Sabine H. L. Klapp
\n<\/i>Phys. Rev. E 86, 061135 (2012)<\/a>, arXiv:1209.1504<\/a><\/p>\n

<\/a>[54] Reverse quantum state engineering using electronic feedback loops
\n<\/b>G. Kiesslich, C. Emary, G. Schaller, T. Brandes
\n<\/i>New J. Phys. 14 123036 (2012)<\/a>, arXiv:1209.1226<\/a><\/p>\n

<\/a>[53] Spin entangled two-particle dark state in quantum transport through coupled quantum dots
\n<\/b>Christina P\u00f6ltl, Clive Emary, Tobias Brandes
\n<\/i>Phys. Rev. B 87, 045416 (2013)<\/a>, arXiv:1209.0992<\/a><\/p>\n

<\/a>[52] Collective strong coupling in multimode cavity QED
\n<\/b>A. Wickenbrock, M. Hemmerling, G. R. M. Robb, C. Emary, and F. Renzoni<\/i>
\nPhys. Rev. A 87, 043817 (2013)<\/a>
\n
\n[51] Nonequilibrium Quantum Phase Transitions in the Ising Model
\n<\/b>V. M. Bastidas, C. Emary, G. Schaller, T. Brandes
\n<\/i>Phys. Rev. B 86, 063627 (2012)<\/a>, arXiv:1207.5242<\/a><\/p>\n

<\/a>[50] Delayed feedback control in quantum transport
\n<\/b>Clive Emary
\n<\/i>Phil. Trans. R. Soc. A 371 1999 (2013)<\/a>, arXiv:1207.2910<\/a><\/p>\n

<\/a>[49] A diagrammatic description of the equation of motion, current, and noise within the second-order von Neumann approach
\n<\/b>O. Karlstr\u00f6m, C. Emary, P. Zedler, J. N. Pedersen, C. Bergenfeldt, P. Samuelsson, T. Brandes, and A. Wacker
\n<\/i>J. Phys. A: Math. Theor. 46, 065301 (2013)<\/a>, arXiv:1206.1744<\/a><\/p>\n

<\/a>[48] Thermal phase transitions for Dicke-type models in the ultra-strong coupling limit
\n<\/b>M. Aparicio Alcalde, M. Bucher, C. Emary, and T. Brandes
\n<\/i>Phys. Rev. E 86, 012101 (2012)<\/a>, arXiv:1204.2271<\/a><\/p>\n

<\/a>[47] Leggett-Garg inequalities for the statistics of electron transport
\n<\/b>Clive Emary
\n<\/i>Phys. Rev. B 86, 085418 (2012)<\/a>, arXiv:1201.4922<\/a><\/p>\n

<\/a>[46] Bunching and anti-bunching in electronic transport
\n<\/b>C. Emary, C. P\u00f6ltl, A. Carmele, J. Kabuss, A. Knorr, T. Brandes
\n<\/i>Phys. Rev. B 85, 165417 (2012)<\/a>, arXiv:1201.6323<\/a><\/p>\n

<\/a>[45] Noise calculations within the second-order von Neumann approach
\n<\/b>Philipp Zedler, Clive Emary, Tobias Brandes, Tomas Novotny
\n<\/i>Phys. Rev. B 84, 233303 (2011)<\/a>, arXiv:1110.3253<\/a><\/p>\n

<\/a>[44] Phase transitions and dark-state physics in two-color superradiance
\n<\/b>Mathias Hayn, Clive Emary, Tobias Brandes
\n<\/i>Phys. Rev. A 84, 053856 (2011)<\/a>, arXiv:1109.2456<\/a><\/p>\n

<\/a>[43] Non-equilibrium Quantum Phase Transitions in the Dicke Model<\/b>
\nV. M. Bastidas, C. Emary, B. Regler, and T. Brandes<\/i>
\nPhys. Rev. Lett. 108, 043003 (2012)<\/a>, arXiv:1108.2987<\/a><\/p>\n

<\/a>[42] Quantum versus classical counting in nonMarkovian master equations
\n<\/b>Clive Emary and Ramon Aguado
\n<\/i>Phys. Rev. B 84, 085425 (2011)<\/a>, arXiv:1106.5219<\/a><\/p>\n

<\/a>[41] Probing the power of an electronic Maxwell’s demon: Single-electron transistor monitored by a quantum point contact
\n<\/b>Gernot Schaller, Clive Emary, Gerold Kiesslich, Tobias Brandes
\n<\/i>Phys. Rev. B 84, 085418 (2011)<\/a>, arXiv:1106.4670<\/a><\/p>\n

<\/a>[40] Limit-Cycles and Chaos in the Current Through a Quantum Dot
\n<\/b>Carlos L\u00f3pez-Mon\u00eds, Clive Emary, Gerold Kiesslich, Gloria Platero, Tobias Brandes
\n<\/i>Phys. Rev. B 85, 045301 (2012)<\/a>, arXiv:1104.3995<\/a><\/p>\n

<\/a>[39] Feedback stabilization of pure states in quantum transport
\n<\/b>Christina P\u00f6ltl, Clive Emary, and Tobias Brandes
\n<\/i>Phys. Rev. B 84, 085302 (2011)<\/a>, arXiv:1103.2710<\/a><\/p>\n

<\/a>[38] Charge Qubit Purification by an Electronic Feedback Loop<\/b>
\nG. Kiesslich, G. Schaller, C. Emary, and T. Brandes
\n<\/i>Phys. Rev. Lett. 107, 050501 (2011)<\/a>, arXiv:1102.3771<\/a><\/p>\n

<\/a>[37] Non-Markovian effects in the Quantum noise of interacting nanostructures
\n<\/b>D. Marcos, C. Emary, T. Brandes, and R. Aguado
\n<\/i>Phys. Rev. B 83, 125426 (2011)<\/a>, arXiv:1006.5586<\/a><\/p>\n

<\/a>[36] Self-consistent electron counting statistics
\n<\/b>Clive Emary
\n<\/i>J. Phys.: Condens. Matter 23 025304 (2011)<\/a>, arXiv:1004.5532<\/a><\/p>\n

<\/a>[35] Finite-frequency counting statistics of electron transport: Markovian Theory
\n<\/b>D. Marcos, C. Emary, T. Brandes, and R. Aguado
\n<\/i>New J. Phys. 12, 123009 (2010)<\/a>, arXiv:1004.1572<\/a><\/p>\n

<\/a>[34] Distinguishing quantum and classical transport through nanostructures
\n<\/b>Neill Lambert, Clive Emary, Yueh-Nan Chen, Franco Nori
\n<\/i>Phys. Rev. Lett. 105, 176801 (2010)<\/a>, arXiv:1002.3020<\/a><\/p>\n

<\/a>[33] Entanglement and parametric resonance in driven quantum systems<\/b>
\nV. M. Bastidas, J. H. Reina, C. Emary, and T. Brandes
\n<\/i>Phys. Rev. A 81, 012316 (2010)<\/a>, arXiv:0910.1600<\/a><\/p>\n

<\/a>[32] Three-level mixing and dark states in transport through quantum dots
\n<\/b>Clive Emary, Christina P\u00f6ltl, and Tobias Brandes
\n<\/i>Phys. Rev. B 80, 235321 (2009)<\/a>, arXiv:0908.3935<\/a><\/p>\n

<\/a>[31] Quantum impurity models with the Coupled Cluster Method
\n<\/b>Jin-Jun Liang, Clive Emary, and Tobias Brandes
\n<\/i>Commun. Theor. Phys. 54, 509 (2010)<\/a>, arXiv:0906.4684<\/a><\/p>\n

<\/a>[30] Spin Spectroscopy via Single-Electron Magnetotunneling
\n<\/b>Gerold Kie\u00dflich, Gernot Schaller, Clive Emary, and Tobias Brandes
\n<\/i>Appl. Phys. Lett. 95, 152104 (2009), <\/a>arXiv:0906.1986<\/p>\n

<\/a>[29] Measuring the Entanglement between Double Quantum Dot Charge Qubits
\n<\/b>C. Emary
\n<\/i>Phys. Rev. B 80, 161309(R) (2009)<\/a>, arXiv:0905.2269<\/a><\/p>\n

<\/a>[28] Two-Particle Dark State in the Transport through a Triple Quantum Dot<\/b>
\nChristina P\u00f6ltl, C. Emary, and T. Brandes
\nPhys. Rev. B 80, 115313 (2009)<\/a>, arXiv:0905.2087<\/a><\/p>\n

<\/a>[27] Counting statistics of cotunneling electrons
\n<\/b>C. Emary
\nPhys. Rev. B 80, 235306 (2009)<\/a>, arXiv:0902.3544<\/a><\/p>\n

<\/a>[26] Weak coupling approximations in non-Markovian Transport
\n<\/b>P. Zedler, G. Schaller, G. Kie\u00dflich, C. Emary, and T. Brandes
\n<\/i>Phys. Rev. B 80, 045309 (2009)<\/a>, arXiv:0902.2118<\/a><\/p>\n

<\/a>[25] Quantum dynamics in nonequilibrium environments
\n<\/b>C. Emary
\n<\/i>Phys. Rev. A 78, 032105 (2008)<\/a>, arXiv:0804.4869<\/a><\/p>\n

<\/a>[24] Adiabatic optical entanglement between electron spins in separate quantum dots
\n<\/b>S. K. Saikin, C. Emary, D. G. Steel, L. J. Sham
\n<\/i>Phys. Rev. B 78, 235314 (2008)<\/a>, arXiv:0802.1527<\/a><\/p>\n

<\/a>[23]Fast Spin State Initialization in a Singly Charged InAs-GaAs Quantum Dot by Optical Cooling
\n<\/b>Xiaodong Xu, Yanwen Wu, Bo Sun, Qiong Huang, Jun Cheng, D. G. Steel, A. S. Bracker, D. Gammon, C.Emary, and L. J. Sham
\n<\/i>Phys. Rev. Lett. 99, 097401 (2007)<\/a><\/p>\n

<\/a>[22] Dark states in the magnetotransport through triple quantum dots<\/b>
\nC. Emary
\n<\/i>Phys. Rev. B 76, 245319 (2007)<\/a>, arXiv:0705.2934<\/a><\/p>\n

<\/a>[21] Frequency-dependent counting statistics in interacting nanoscale conductors<\/b>
\nC. Emary, D. Marcos, R. Aguado, and T. Brandes<\/i>
\nPhys. Rev. B 76, 161404(R) (2007)<\/a>, cond-mat\/0703781<\/a><\/p>\n

<\/a>[20] Optically-controlled logic gates for two spin qubits in vertically-coupled quantum dots<\/b>
\nC. Emary and L. J. Sham<\/i>
\nPhys. Rev. B 75, 125317 (2007)<\/a>, cond-mat\/0609094<\/a><\/p>\n

<\/a>[19] Optically controlled single-qubit rotations in self-assembled InAs quantum dots<\/b>
\nC. Emary and L. J. Sham<\/i>
\nJ. Phys.: Condens. Matter 19, 056203 (2007)<\/a>, cond-mat\/0608518<\/a><\/p>\n

<\/a>[18] Fast Initialization of the Spin State of an Electron in a Quantum Dot in the Voigt Configuration<\/b>
\nC. Emary, X. Xu, D. G. Steel, S. Saikin, and L. J. Sham<\/i>
\nPhys. Rev. Lett. 98, 047401 (2007)<\/a>, cond-mat\/0608225<\/a><\/p>\n

<\/a>[17] All Electronic coherent population trapping in quantum dots<\/b>
\nB. Michaelis, C. Emary, and C. W. J. Beenakker<\/i>
\nEurophys. Lett. 73, 677 (2006)<\/a>, cond-mat\/0506005<\/a><\/p>\n

<\/a>[16] Entanglement in quantum catastrophes<\/b>
\nC. Emary, N. Lambert, and T. Brandes<\/i>
\nPhys. Rev. A 71, 062302 (2005)<\/a>, quant-ph\/0503160<\/a><\/p>\n

<\/a>[15] Emission of polarization-entangled microwave photons from a pair of quantum dots<\/b>
\nC. Emary, B. Trauzettel, and C. W. J. Beenakker<\/i>
\nPhys. Rev. Lett. 95, 127401 (2005)<\/a>, cond-mat\/0502550<\/a><\/p>\n

<\/a>[14] Spin-orbit-driven coherent oscillations in a few-electron quantum dot<\/b>
\nS. Debald and C. Emary<\/i>
\nPhys. Rev. Lett. 94, 226803 (2005)<\/a>, cond-mat\/0410714<\/a><\/p>\n

<\/a>[13] Entanglement and entropy in a spin-boson quantum phase transition<\/b>
\nN. Lambert, C. Emary, and T. Brandes<\/i>
\nPhys. Rev. A 71, 053804 (2005), quant-ph\/0405109<\/a><\/p>\n

<\/a>[12] A bipartite class of entanglement monotones for N-qubit pure states<\/b>
\nC. Emary<\/i>
\nJ. Phys. A 37, 8293 (2004)<\/a>, quant-ph\/0405049<\/a><\/p>\n

<\/a>[11] Charge detection enables free-electron quantum computation<\/b>
\nC.W.J. Beenakker, D.P. DiVincenzo, C. Emary, and M. Kindermann<\/i>
\nPhys. Rev. Lett. 93, 020501 (2004)<\/a>, quant-ph\/0401066<\/a><\/p>\n

<\/a>[10] Phase transitions in generalised spin-boson (Dicke) models<\/b>
\nC. Emary and T. Brandes<\/i>
\nPhys. Rev. A 69, 053804 (2004)<\/a>, quant-ph\/0401029<\/a><\/p>\n

<\/a>[9] Relation between entanglement measures and Bell inequalities for three qubits<\/b>
\nC. Emary and C. W. J. Beenakker<\/i>
\nPhys. Rev. A 69, 032317 (2004)<\/a>, quant-ph\/0311105<\/a><\/p>\n

<\/a>[8] Production and detection of three-qubit entanglement in the Fermi sea<\/b>
\nC.W.J. Beenakker, C. Emary, M. Kindermann<\/i>
\nPhys. Rev. B 69, 115320 (2004)<\/a>, cond-mat\/0310496<\/a><\/p>\n

<\/a>[7] Entanglement and the phase transition in single mode superradiance<\/b>
\nN. Lambert, C. Emary, T. Brandes<\/i>
\nPhys. Rev. Lett. 92, 073602 (2004)<\/a>, quant-ph\/0309027<\/a><\/p>\n

<\/a>[6] Proposal for production and detection of entangled electron-hole pairs
\nin a degenerate electron gas<\/b>
\nC.W.J. Beenakker, C. Emary, M. Kindermann, J.L. van Velsen<\/i>
\nPhys. Rev. Lett. 91, 147901 (2003)<\/a>, cond-mat\/0305110
\n<\/a>
\n[5] Chaos and the quantum phase transition in the Dicke model<\/b>
\nC. Emary and T. Brandes<\/i>
\nPhys. Rev. E 67, 066203, (2003)<\/a>, cond-mat\/0301273<\/a><\/p>\n

<\/a>[4]Quantum chaos triggered by precursors of a quantum phase transition:
\nthe Dicke model<\/b>
\nC. Emary and T. Brandes
\n<\/i>Phys. Rev. Lett. 90, 044101 (2003)<\/a>, cond-mat\/0207290<\/a><\/p>\n

<\/a>[3] Exact isolated solutions for the two–photon Rabi Hamiltonian<\/b>
\nC. Emary and R. F. Bishop<\/i>
\nJ. Phys. A 35, 8231 (2002)<\/a>, quant-ph\/0206182<\/a><\/p>\n

<\/a>[2] Bogoliubov Transformations and exact isolated solutions for simple non-adiabatic Hamiltonians<\/b>
\nC. Emary and R. F. Bishop<\/i>
\nJ. Math. Phys. 43, 3916 (2002)<\/a>, quant-ph\/0112061<\/a><\/p>\n

<\/a>[1] Time-evolution of the Rabi Hamiltonian from the unexcited vacuum<\/b>
\nR. F. Bishop and C. Emary<\/i>
\nJ. Phys. A 34, 5635, (2001)<\/a>, quant-ph\/0209102<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"

[98] Ternary network models for disturbed ecosystems Kieran Peel, Darren Evans and Clive Emary R. Soc. Open Sci. 9 220619 (2022) [97] Network science: Applications for sustainable agroecosystems and food security Fredric M. Windsor, et al. Perspectives in Ecology and Conservation (2022) [96] Stability-instability transition in tripartite merged ecological networks Clive Emary and Anne-Kathleen Malchow … Continue reading Publications<\/span> →<\/span><\/a><\/p>\n","protected":false},"author":1390,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"open","template":"","meta":{"footnotes":""},"class_list":["post-17","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/pages\/17","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/users\/1390"}],"replies":[{"embeddable":true,"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/comments?post=17"}],"version-history":[{"count":63,"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/pages\/17\/revisions"}],"predecessor-version":[{"id":227,"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/pages\/17\/revisions\/227"}],"wp:attachment":[{"href":"https:\/\/www.staff.ncl.ac.uk\/clive.emary\/wp-json\/wp\/v2\/media?parent=17"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}