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1 cs, complex numbers are used to describe the wavefunction.
2 pairs, with Fermi surface nodes in the pair wavefunction.
3 to the near-field component of the photon's wavefunction.
4 eak measurements of the momentum in a vortex wavefunction.
5 d by Anderson localization of the electronic wavefunction.
6 result of the presence of the excited state wavefunction.
7 an efficient way to record the large system wavefunctions.
8 ed by the topological properties of the bulk wavefunctions.
9 eoretically using Gutzwiller-projected trial wavefunctions.
10 king and minimizes the interlayer overlap of wavefunctions.
11 ying the pseudospin character of the carrier wavefunctions.
12 irect signatures of correlated many-electron wavefunctions.
13 esponding hydrogen and deuterium vibrational wavefunctions.
14 antitative description of their ground state wavefunctions.
15 product mixed electronic-proton vibrational wavefunctions.
16 (a geometric quantum phase) of the electron wavefunction--a consequence of the exceptional topology
19 ed forms, spikes appearing in the condensate wavefunction and oscillating remnant condensates that su
20 xperimentally explore collapse models of the wavefunction and the potential for mechanical-resonator-
22 generates nanoscale views of the electronic wavefunctions and magnetic order at topological surfaces
23 erties define the nature of the ground state wavefunctions and so serve as a sensitive and quantitati
24 essing the complex interplay between quantum wavefunctions and various factors such as dimensionality
25 on an explicit ansatz for the many-electron wavefunctions and, hence, potentially more accurate--hav
26 sociation spectra; these probe the molecular wavefunction, and yield binding energies that are consis
27 hods, so we have resorted to multi-reference wavefunction approaches, the entry level of which is the
29 y another, are excited Rydberg states, where wavefunctions are expanded from their ground-state exten
30 le-domain heterostructures, however, carrier wavefunctions are more complex and still not well unders
33 eoretically recasting a phase in the qubit's wavefunction as a topological winding number, we can sat
34 demonstrates that modern implementations of wavefunction-based correlated methods are playing an inc
35 to appreciable overlap of quantum mechanical wavefunctions between neighboring delta-doped layers.
36 tainty principle governs the dynamics of the wavefunction by enforcing a lower bound on the measureme
37 control over the spatial distribution of the wavefunction can be obtained by increasing the number of
38 quantum systems--notably in photonics, where wavefunctions can be observed directly--provide versatil
41 In quantum mechanics, measurements cause wavefunction collapse that yields precise outcomes, wher
42 amics make a smooth transition from standard wavefunction collapse to localized persistent diffusion
43 surement dynamics, typically associated with wavefunction collapse, and unitary evolution of the quan
44 In superconducting Rashba metals a pairing wavefunction constructed from these complex spin structu
46 uction reveals a remarkable phenomenon where wavefunction delocalization and Coulomb gap collapse are
48 s to T1 states can be strongly suppressed by wavefunction delocalization, allowing for the dissociati
49 show how interference effects of the quantum wavefunction describing multiple electrons can be used t
50 strating that strong quantum confinement and wavefunction engineering in heterostructured nanocrystal
51 refore motivate the need to analyse electron wavefunctions, especially their wavefronts, to obtain in
52 factorized into a product of single-particle wavefunctions, even when the constituent particles are e
53 o atoms into the same physical location, the wavefunction exchange symmetry of these identical bosons
54 ypically only a small fraction of a particle wavefunction extends into the tunneling region, we prese
55 e of Wannier type, meaning that each exciton wavefunction extends over multiple unit cells, but with
57 of freedom cannot be written as a product of wavefunctions for each degree of freedom-becomes visible
58 c groups and complex global migration of the wavefunction from the outer to inner ring, which may hav
61 ameters and to show it depends explicitly on wavefunctions in addition to standard band structure.
64 demonstrate the coherent control of impurity wavefunctions in the most ubiquitous donor in a semicond
65 spectroscopic measurements have only probed wavefunctions indirectly, preventing direct experimental
66 e advantage that the reconstructed exit-face wavefunction is free of the aberrations of the objective
67 ifferent sequences, we find that the polaron wavefunction is predominantly on one of the two chains,
69 tramolecular redistribution of excited state wavefunction, leading, in turn, to different time-scales
71 m mechanical effects-entanglement, where the wavefunction of a system with several degrees of freedom
72 in recent years has the ability to shape the wavefunction of EBeams (Electron-Beams) become experimen
74 nfinement in semiconductors can compress the wavefunctions of band electrons and holes to nanometre-s
75 hen interacting with magnetic materials, the wavefunctions of such electrons are inherently modified.
77 normally obscured in structures in which the wavefunctions of the electron and trapped hole spatially
78 tum model confirms the delocalization of the wavefunctions of the hybridized states and its effect on
79 the spatial properties of the excited-state wavefunctions of the whole bacteriochlorophyll complex.
81 re considered 'artificial atoms' because the wavefunctions of their charge carriers resemble those of
82 e atomic-resolution complex image (exit-face wavefunction) of a small particle lying on a thin carbon
84 sions and time, we show that imprinting such wavefunctions on electron pulses leads to shape-preservi
85 ill operate on overlapping electron and hole wavefunctions on the same polymer chain at their capture
86 tra reveal projections of the double-exciton wavefunctions onto a basis of direct products of single
88 als can be used to manipulate carrier-Mn(2+) wavefunction overlap and the sp-d exchange parameters th
89 tributed by the improvement in electron-hole wavefunction overlap, as compared to that of conventiona
90 actions, such as those requiring substantial wavefunction overlap, can alleviate these detrimental ef
91 systems, where contact interactions require wavefunction overlap, effective spin interactions on a l
92 tigation also reveals that the electron-hole wavefunction overlaps are remarkably large in the InGaN
93 re, our study reveals that the electron-hole wavefunction overlaps in the AlN/GaN DA structure can be
98 ps of the hydrogen and deuterium vibrational wavefunctions strongly impacts the magnitude of the KIE
99 Quantum mechanics allows for many-particle wavefunctions that cannot be factorized into a product o
100 of the mechanisms based on delocalized hole wavefunctions that had been investigated, both experimen
101 lian, are characterized by excitations whose wavefunctions undergo nontrivial statistical transformat
102 re the dynamical evolution of the two-photon wavefunction using time-resolved quantum state tomograph
103 using only the scattered part of each atom's wavefunction, we precisely measure the difference of the
104 nstrate that knotting also occurs in quantum wavefunctions, where the tangled filaments are vortices
105 graphic technique to manipulate the electron wavefunction, which gives free electrons an additional u
106 e are imprinted on the recoiling part of the wavefunction, which moves towards the second condensate.
107 f its electronic states in terms of envelope wavefunctions whose energy, time, and length scales are
108 iple carbon sublattices endow the electronic wavefunctions with pseudospin, a lattice analogue of the
110 ield leads to a displacement of the electron wavefunction within the quantum well, and because the el
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