Abstract is: Jeremy Mark Hutson is noted for his research into ultra cold physics and he heads up the Cold Molecules Theory research group. His research led to his appointment as a Fellow of the Royal SocietyHe is a fellow of the Institute of Physics and is currently Professor of Chemistry and Physics at Durham University.
| human | Q5 |
| P6178 | Dimensions author ID | 0743265340.49 |
| P2070 | Fellow of the Royal Society ID | 11675 |
| P8446 | Gateway to Research person ID | D249029F-DFBF-4670-B6B7-A353E4344DCB |
| P2671 | Google Knowledge Graph ID | /g/11c72qlgtw |
| P1960 | Google Scholar author ID | 5jpoY_QAAAAJ |
| P269 | IdRef ID | 129913103 |
| P496 | ORCID iD | 0000-0002-4344-6622 |
| P3829 | Publons author ID | 2723478 |
| P1053 | ResearcherID | F-4748-2012 |
| P6023 | ResearchGate contributions ID | 9896234 |
| P1153 | Scopus author ID | 7202644008 |
| P10861 | Springer Nature person ID | 0743265340.49 |
| P214 | VIAF ID | 198917667 |
| P166 | award received | Corday-Morgan Prize | Q898961 |
| Kołos Medal | Q3332223 | ||
| Fellow of the Royal Society | Q15631401 | ||
| Tilden Prize | Q18560214 | ||
| Joseph Thomson Medal and Prize | Q20749254 | ||
| P69 | educated at | University of Oxford | Q34433 |
| P108 | employer | Pembroke College | Q82606 |
| Durham University | Q458393 | ||
| Pembroke College | Q956501 | ||
| University of Waterloo | Q1049470 | ||
| P734 | family name | Hutson | Q39324298 |
| Hutson | Q39324298 | ||
| Hutson | Q39324298 | ||
| P735 | given name | Jeremy | Q1514341 |
| Jeremy | Q1514341 | ||
| Mark | Q13610143 | ||
| Mark | Q13610143 | ||
| P463 | member of | Royal Society | Q123885 |
| P106 | occupation | physicist | Q169470 |
| chemist | Q593644 | ||
| P21 | sex or gender | male | Q6581097 |
| Q57961330 | A classical trajectory study of Ar+Ar2 collisions: Phase space structures in three degrees of freedom |
| Q57961402 | A comparison of the vibrational predissociation rates in the rare-gas–ethylene clusters |
| Q57961305 | A failing of coupled-states calculations for inelastic and pressure-broadening cross sections: Calculations on CO2–Ar |
| Q57961457 | A new approach to perturbation theory for breakdown of the Born-Oppenheimer approximation |
| Q57961366 | A new direct infrared laser absorption method for state‐to‐state rotational energy transfer in crossed supersonic jets: Experimental results and quantum scattering analysis for Ar+CH4 |
| Q57961410 | A semiempirical model for atom-surface dispersion coefficients |
| Q57961377 | A spectroscopic puzzle in ArHF solved: The test of a new potential |
| Q57961333 | A systematic model potential for Li+-H2O |
| Q57961391 | A theoretical study of the Ar2HCl van der Waals cluster |
| Q57961271 | Ab initio potential energy surfaces, bound states, and electronic spectrum of the Ar–SH complex |
| Q57961441 | Accidental predissociation in lithium dimer: A theoretical investigation |
| Q57961325 | An evaluation of existing potential energy surfaces for CO2–Ar: Pressure broadening and high‐resolution spectroscopy of van der Waals complexes |
| Q57961230 | An ultracold high-density sample of rovibronic ground-state molecules in an optical lattice |
| Q57961443 | Anisotropic intermolecular forces |
| Q57961445 | Anisotropic intermolecular forces |
| Q57961427 | Anisotropic intermolecular forces from Hartree-Fock plus damped dispersion (HFD) calculations |
| Q57961286 | Anisotropic intermolecular forces. I. Rare gas—hydrogen chloride systems |
| Q57961392 | Anisotropic intermolecular potentials. III. Rare‐gas–hydrogen bromide systems |
| Q57961174 | Approach to chaos in ultracold atomic and molecular physics: Statistics of near-threshold bound states for Li+CaH and Li+CaF |
| Q57961279 | ArnHF van der Waals clusters revisited: II. Energetics and HF vibrational frequency shifts from diffusion Monte Carlo calculations on additive and nonadditive potential-energy surfaces for n=1-12 |
| Q57961346 | Atom-Molecule van der Waals Complexes Containing Open-Shell Atoms. 2. The Bound States of Cl-HCl |
| Q49831133 | Atomic Clock Measurements of Quantum Scattering Phase Shifts Spanning Feshbach Resonances at Ultralow Fields |
| Q57961349 | Atom‐spherical top van der Waals complexes: A theoretical study |
| Q57961386 | Atom–asymmetric top van der Waals complexes: Angular momentum coupling in Ar–H2O |
| Q57961345 | Atom–molecule van der Waals complexes containing open‐shell atoms. I. General theory and bending levels |
| Q57961252 | Avoided crossings between bound states of ultracold cesium dimers |
| Q125865820 | Bose-Einstein condensation of non-ground-state caesium atoms |
| Q57961351 | Bound‐state wave functions from coupled channel calculations using log‐derivative propagators: Application to spectroscopic intensities in Ar–HF |
| Q57188076 | Calculating energy levels of isomerizing tetra-atomic molecules. I. The rovibrational bound states of Ar2HF |
| Q45289664 | Calculating energy levels of isomerizing tetra-atomic molecules. II. The vibrational states of acetylene and vinylidene |
| Q57961334 | Calculating nuclear quadrupole coupling constants for van der Waals complexes |
| Q57961337 | Calculations of line width and shift cross sections for HC1 in Ar |
| Q57961338 | Calculations of the spectra of rare gas dimers and trimers: Implications for additive and nonadditive intermolecular forces in Ne2–Ar, Ne2–Kr, Ne2–Xe, Ar2–Ne, Ar3, Ar2–Kr and Ar2–Xe |
| Q57961451 | Centrifugal distortion constants for diatomic molecules: an improved computational method |
| Q57961163 | Characterizing Feshbach resonances in ultracold scattering calculations |
| Q57961429 | Close‐coupling calculations of transport and relaxation cross sections for H2 in Ar |
| Q57961404 | Close‐coupling calculations of transport and relaxation cross sections for H2in Ar |
| Q57961288 | Clusters containing open-shell molecules. II. Equilibrium structures of ArnOH Van der Waals clusters (X2Π, n=1 to 15) |
| Q57961290 | Clusters containing open-shell molecules. III. Quantum five-dimensional/two-surface bound-state calculations on ArnOH van der Waals clusters (X2Π, n=4 to 12) |
| Q42661621 | Clusters containing open-shell molecules: minimum-energy structures and low-lying isomers of ArnCH (X 2 pi), n = 1 to 15. |
| Q57961209 | Cold and ultracold NH-NH collisions in magnetic fields |
| Q57961210 | Cold and ultracold NH–NH collisions: The field-free case |
| Q57961183 | Cold atomic and molecular collisions: approaching the universal loss regime |
| Q57961262 | Cold collisions between OH and Rb: The field-free case |
| Q57961211 | Cold collisions of N (4S) atoms and NH (3Σ) molecules in magnetic fields |
| Q57961213 | Cold collisions of an open-shell S-state atom with a 2Π molecule: N(4S) colliding with OH in a magnetic field |
| Q57961188 | Collision cross sections for the thermalization of cold gases |
| Q57961239 | Conical Intersections in Laboratory Coordinates with Ultracold Molecules |
| Q57961190 | Contrasting the wide Feshbach resonances inLi6andLi7 |
| Q57961175 | Controlling the rotational and hyperfine state of ultracoldRb87Cs133molecules |
| Q57961396 | Coupled channel bound state calculations: Calculating expectation values without wavefunctions |
| Q57961411 | Coupled channel calculations on the vibrational predissociation of the ethylene dimer |
| Q57961353 | Coupled channel methods for solving the bound-state Schrödinger equation |
| Q57961178 | Creating Feshbach resonances for ultracold molecule formation with radio-frequency fields |
| Q57161799 | Creation of ultracold ^{87}Rb^{133}Cs molecules in the rovibrational ground state |
| Q57961179 | Deviations from Born-Oppenheimer mass scaling in spectroscopy and ultracold molecular physics |
| Q57961453 | Direct summation over vibrational levels: Λ doubling in HF+ |
| Q57961241 | Dramatic Reductions in Inelastic Cross Sections for Ultracold Collisions near Feshbach Resonances |
| Q57961414 | Dynamics of physisorption for the H2,D2Cu(100) and H2Ag(111) systems |
| Q57961215 | Effect of hyperfine interactions on ultracold molecular collisions: NH(3Σ−) with Mg(1S) in magnetic fields |
| Q57961317 | Energy corrected sudden calculations of linewidths and line shapes based on coupled states cross sections: The test case of CO2–argon |
| Q57961388 | Exact and approximate calculations for the effect of potential anisotropy on integral and differential cross-sections: Ar–N2rotationally inelastic scattering |
| Q57961263 | Feshbach resonances in ultracold atomic and molecular collisions: threshold behaviour and suppression of poles in scattering lengths |
| Q57961193 | Feshbach resonances, molecular bound states, and prospects of ultracold-molecule formation in mixtures of ultracold K and Cs |
| Q62582374 | Feshbach resonances, weakly bound molecular states, and coupled-channel potentials for cesium at high magnetic fields |
| Q57961454 | High resolution radiofrequency spectroscopy of Ar⋅⋅⋅HCl |
| Q57961243 | Hyperfine energy levels of alkali-metal dimers: Ground-state homonuclear molecules in magnetic fields |
| Q57961255 | Hyperfine energy levels of alkali-metal dimers: Ground-state polar molecules in electric and magnetic fields |
| Q57961232 | Hyperfine structure in the microwave spectra of ultracold polar molecules |
| Q57961161 | Hyperfine structure of 2Σ molecules containing alkaline-earth-metal atoms |
| Q57961166 | Hyperfine structure of alkali-metal diatomic molecules |
| Q57961320 | I-NoLLS: A program for interactive nonlinear least-squares fitting of the parameters of physical models |
| Q57961407 | Improved potential energy surfaces for the interaction of H2with Ar, Kr, and Xe |
| Q57961167 | Inelastic losses in radio-frequency-dressed traps for ultracold atoms |
| Q57961216 | Interaction between LiH molecule and Li atom from state-of-the-art electronic structure calculations |
| Q49249631 | Interaction of NH(X3Sigma-) molecules with rubidium atoms: implications for sympathetic cooling and the formation of extremely polar molecules |
| Q57957581 | Interactions and dynamics in Li+Li2 ultracold collisions |
| Q57961390 | Intermolecular Forces From The Spectroscopy Of Van Der Waals Molecules |
| Q57961300 | Intermolecular potential energy surfaces and bound states in F–HF |
| Q57961459 | Intermolecular potential energy surfaces for Kr·HCl and Ar·HBr |
| Q57961409 | International electronic mail |
| Q57961168 | Interspecies thermalization in an ultracold mixture of Cs and Yb in an optical trap |
| Q57961218 | Large Effects of Electric Fields on Atom-Molecule Collisions at Millikelvin Temperatures |
| Q57961257 | Large-amplitude quantum mechanics in polyatomic hydrides. II. A particle-on-a-sphere model for XHn (n=4,5) |
| Q57961322 | Line shape, transport and relaxation properties from intermolecular potential energy surfaces: The test case of CO2–Ar |
| Q89935206 | Long Rotational Coherence Times of Molecules in a Magnetic Trap |
| Q57961272 | Long range intermolecular forces in triatomic systems: connecting the atom–diatom and atom–atom–atom representations |
| Q57961244 | Low-energy collisions ofNH3andND3with ultracold Rb atoms |
| Q57961206 | Magnetically Tunable Feshbach Resonances in Ultracold Li-Yb Mixtures |
| Q57961247 | Manipulating ultracold polar molecules with microwave radiation: The influence of hyperfine structure |
| Q57961180 | Measurement of the binding energy of ultracoldRb87Cs133molecules using an offset-free optical frequency comb |
| Q57961367 | Methods for calculating the bound state energies of van der Waals trimers: Applications to Ar3 |
| Q58590005 | Microwave Shielding of Ultracold Polar Molecules |
| Q96026859 | Microwave coherent control of ultracold ground-state molecules formed by short-range photoassociation |
| Q57961293 | Microwave electronic spectrum of the Ne⋯Ne+ long-range complex: The interaction potential |
| Q57803614 | Microwave spectroscopy and interaction potential of the long‐range He...Ar+ion |
| Q56776320 | Microwave spectroscopy and interaction potential of the long‐range He⋯Kr+ ion: An example of Hund’s case (e) |
| Q57961186 | Modeling sympathetic cooling of molecules by ultracold atoms |
| Q57961265 | Molecular collisions in ultracold atomic gases |
| Q57961274 | Molecule formation in ultracold atomic gases |
| Q57961306 | Morphing ab initio potentials: A systematic study of Ne–HF |
| Q57961298 | Morphing the He–OCS intermolecular potential |
| Q57961221 | Multichannel quantum defect theory for cold molecular collisions |
| Q57961295 | Near-dissociation states and coupled potential curves for the HeN+ complex |
| Q57188063 | New vibration–rotation code for tetraatomic molecules exhibiting wide-amplitude motion: WAVR4 |
| Q57961324 | Non-additive intermolecular forces from the spectroscopy of Van der Waals trimers: A comparison of Ar2–HF and Ar2–HCl, including H/D isotope effects |
| Q57961357 | Non-additive intermolecular forces from the spectroscopy of Van der Waals trimers: the effect of monomer vibrational excitation in Ar2–HF and Ar2–HCl |
| Q57961355 | Non-additive intermolecular forces from the spectroscopy of van der Waals trimers: far-infrared spectra and calculations on Ar2-DCl |
| Q57961340 | Nonadditive intermolecular forces from the spectroscopy of van der Waals trimers: A theoretical study ofAr2-HF |
| Q57961368 | Nonadditive intermolecular forces from the spectroscopy of van der Waals trimers: Calculations on Ar2–HCl |
| Q57961308 | Nonadditive intermolecular forces in Arn–HF van der Waals clusters: Effects on the HF vibrational frequency shift |
| Q57961160 | Observation of Feshbach resonances between alkali and closed-shell atoms |
| Q56519139 | Observation of a microwave spectrum of the long-range He … H2+ complex |
| Q57961171 | Observation of interspecies Feshbach resonances in an ultracold K39−Cs133 mixture and refinement of interaction potentials |
| Q27450069 | Observation of the Second Triatomic Resonance in Efimov’s Scenario |
| Q57961358 | On the choice of inertial axes for interpreting spectroscopic properties of van der Waals complexes |
| Q57961393 | On the coupled‐channel calculation of bound states for trimeric systems using hyperspherical coordinates |
| Q57961361 | On the rotational constants of floppy molecules |
| Q57961222 | Optically induced conical intersections in traps for ultracold atoms and molecules |
| Q57961415 | Pairwise-additive models for atom-surface interaction potentials: An ab initio study of He-LiF |
| Q57961379 | Parity doubling in open-shell van der Waals complexes |
| Q57961371 | Physical origin of oscillations in the three‐dimensional collision amplitudes of heavy–light–heavy systems. Semiclassical quantization of chaotic scattering |
| Q57961282 | Potential energy surfaces and bound states for the open-shell van der Waals cluster Br–HF |
| Q57961301 | Potential energy surfaces and properties of the Br–HBr complex |
| Q57961373 | Potential energy surfaces for Ar–OH (X 2Π) obtained by fitting to high‐resolution spectroscopy |
| Q51231606 | Precise characterization of 6Li Feshbach resonances using trap-sideband-resolved RF spectroscopy of weakly bound molecules. |
| Q57961309 | Predictions of microwave and far-infrared transitions in He-H+2 |
| Q57961434 | Predissociation of HD–Ar van der Waals molecules by internal rotation |
| Q57961447 | Predissociation of weak-anisotropy Van der Waals molecules. Theory, approximations and practical predictions |
| Q36067913 | Production of Ultracold (87) Rb(133) Cs in the Absolute Ground State: Complete Characterisation of the Stimulated Raman Adiabatic Passage Transfer. |
| Q57961249 | Production of Ultracold NH Molecules by Sympathetic Cooling with Mg |
| Q57961194 | Production of optically trappedRbCs87Feshbach molecules |
| Q57961310 | Properties of H+2 relevant to the He-H2 intermolecular potential: asymptotically increasing multipole moments, polarizabilities and dispersion coefficients |
| Q57961259 | Prospects for producing ultracoldNH3molecules by sympathetic cooling: A survey of interaction potentials |
| Q47620056 | Prospects for sympathetic cooling of polar molecules: NH with alkali-metal and alkaline-earth atoms--a new hope |
| Q57961202 | Prospects of forming ultracold molecules in2Σstates by magnetoassociation of alkali-metal atoms with Yb |
| Q57961416 | Quadrupolar contributions to the atom-surface Van Der Waals interaction |
| Q57957610 | Quantum Dynamics of UltracoldNa+ Na2Collisions |
| Q57961182 | Quantum chaos in ultracold collisions betweenYb(1S0)andYb(3P2) |
| Q57961195 | Reactions between cold methyl halide molecules and alkali-metal atoms |
| Q57961233 | Reactions of ultracold alkali-metal dimers |
| Q57961303 | Regular and irregular vibrational states: Localized anharmonic modes and transition-state spectroscopy of Na3 |
| Q57961312 | Regular and irregular vibrational states: Localized anharmonic modes in Ar3 |
| Q57961276 | Roger E. Miller |
| Q57961436 | Rotational predissociation of the Ar⋅HCl van der Waals complex: Close‐coupled scattering calculations |
| Q57961326 | Rotationally inelastic scattering in CH4+He, Ne, and Ar: State‐to‐state cross sections via direct infrared laser absorption in crossed supersonic jets |
| Q57961437 | Selective adsorption resonances in the scattering of helium atoms from xenon coated graphite: Close‐coupling calculations and potential dependence |
| Q57961363 | Signatures of large amplitude motion in a weakly bound complex: High‐resolution IR spectroscopy and quantum calculations for HeCO2 |
| Q57961397 | Single-step methods for calculating activation parameters from raw kinetic data |
| Q57961364 | Spectral line shape parameters for HF in a bath of Ar are accurately predicted by a potential inferred from spectra of the van der Waals dimer |
| Q57961461 | Spectroscopic properties and potential surfaces for atom-diatom van der Waals molecules |
| Q91902337 | Sticky collisions of ultracold RbCs molecules |
| Q57961250 | Stimulating the production of deeply bound RbCs molecules with laser pulses: the role of spin–orbit coupling in forming ultracold molecules |
| Q57961204 | Sympathetic cooling of fluorine atoms with ultracold atomic hydrogen |
| Q57961374 | The Ar–HF intermolecular potential: Overtone spectroscopy and ab initio calculations |
| Q57961417 | The atom-surface interaction potential for He-NaCl: A model based on pairwise additivity |
| Q57961419 | The augmented secular equation method for calculating spectra of van der Waals complexes. Application to the infrared spectrum of Ar–HCl |
| Q57961384 | The dynamics of open‐shell Van der Waals complexes |
| Q57961342 | The influence of the ionisation potential on the simulated ion signal from femtosecond pump-probe experiments |
| Q57961327 | The intermolecular potential energy surface for CO2–Ar: Fitting to high‐resolution spectroscopy of Van der Waals complexes and second virial coefficients |
| Q57961456 | The intermolecular potential energy surface of Ar · HC1 |
| Q57961380 | The intermolecular potential of Ar-acetylene. Information from infrared and microwave spectroscopy |
| Q57961399 | The intermolecular potential of Ar–HCl: Determination from high‐resolution spectroscopy |
| Q57961394 | The intermolecular potential of Ne–HCl: Determination from high‐resolution spectroscopy |
| Q57961315 | The potential energy surface and near-dissociation states of He-H2+ |
| Q57961329 | The potential energy surface of He–HCN determined by fitting to high‐resolution spectroscopic data |
| Q57961224 | The prospects of sympathetic cooling of NH molecules with Li atoms |
| Q57961424 | The secular equation/perturbation theory method for calculating spectra of van der Waals complexes |
| Q57961401 | Theoretical studies of van der Waals molecules and intermolecular forces |
| Q57961285 | Three-body nonadditive forces between spin-polarized alkali-metal atoms |
| Q57961197 | Three-body parameter for Efimov states inLi6 |
| Q57961226 | Topical issue on cold quantum matter |
| Q57961319 | Total differential cross sections for Ar–CH4 from an ab initio potential |
| Q57961207 | Towards the production of ultracold ground-state RbCs molecules: Feshbach resonances, weakly bound states, and the coupled-channel model |
| Q57957597 | Ultracold Collisions Involving Heteronuclear Alkali Metal Dimers |
| Q57961278 | Ultracold Rb-OH Collisions and Prospects for Sympathetic Cooling |
| Q57961237 | Ultracold RbSr Molecules Can Be Formed by Magnetoassociation |
| Q57961270 | Ultracold atom-molecule collisions and bound states in magnetic fields: Tuning zero-energy Feshbach resonances inHe−NH(Σ−3) |
| Q57162139 | Ultracold dense samples of dipolar RbCs molecules in the rovibrational and hyperfine ground state |
| Q54514201 | Ultracold hydrogen atoms: a versatile coolant to produce ultracold molecules. |
| Q60171412 | Ultracold molecules for quantum simulation: rotational coherences in CaF and RbCs |
| Q57957600 | Ultracold quantum dynamics: Spin-polarizedK+K2collisions with three identical bosons or fermions |
| Q57957596 | UltracoldLi+Li2Collisions: Bosonic and Fermionic Cases |
| Q57961448 | Use of calculated centrifugal distortion constants (Dν, Hν, Lν and Mν) in the analysis of the B ← X system of I2 |
| Q57961425 | Very low-energy scattering of helium atoms from crystal surfaces. A quantitative comparison between experiment and theory |
| Q57961383 | Vibrational dependence of the anisotropic intermolecular potential of Ar–HF |
| Q57961381 | Vibrational dependence of the anisotropic intermolecular potential of argon-hydrogen chloride |
| Q57961430 | Vibrational predissociation and infrared spectrum of the Ar–HCl van der Waals molecule |
| Q57961439 | Vibrational predissociation of hydrogen, deuterium, and hydrogen deuteride-argon van der Waals molecules |
| Q57961431 | Vibrational predissociation of the Ne–C2H4and Ar–C2H4van der Waals complexes |
| Q57961421 | Vibrational predissociation of the ethylene dimer |
| Q57961344 | Vibrational relaxation of CO (v=1) by inelastic collisions with 3He and 4He |
| Q57961365 | Wavepacket calculations of femtosecond pump-probe experiments on the sodium trimer |
| Q57961172 | ac Stark effect in ultracold polar Rb87Cs133 molecules |
| Q62116468 | bound and field: Programs for calculating bound states of interacting pairs of atoms and molecules |
| Q62116469 | molscat: A program for non-reactive quantum scattering calculations on atomic and molecular collisions |
| Jeremy Hutson | wikipedia |
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