ライフサイエンスコーパス: multipole

1 that from conventional electric and magnetic multipoles.

2 ciated with the familiar charge and magnetic multipoles.

3 eir surface charge distributions in terms of multipoles.

4 tructed from interacting but state-dependent multipoles.

5 se to energy minima found in our Distributed Multipole Analysis based model calculations.

6 ernal ion reservoir consisting of an rf-only multipole and a pair of electrostatic lens elements.

7 t cannot be attributed to magnetic or charge multipoles and can only be explained by the existence of

8 discrete-element model including electrical multipoles and find that infinitesimally small initial c

9 the rf quadrupole ion guide, higher-order rf multipoles and rf stacked ring ion guides, in terms of t

10 d; the limitation is weaker for higher-order multipoles and stacked ring ion guides.

11 omplexes, may be realized using higher-order multipoles and stacked ring ion guides.

12 ovide a good approximation for high-order rf multipoles and stacked ring rf ion guides.

13 exhibits a long-range hidden order in which multipoles are formed from 10-spin loops.

14 Toroidal multipoles are fundamental electromagnetic excitations d

15 wers'), linear quadrupoles (poles) and mixed multipole arrangements ('two tone'), which represent jus

16 thin nematic cells are thus based on elastic multipoles consisting of a particle and nearby defects.

17 Quadrupoles and higher multipoles correspond to fundamental strain-carrying ent

18 Incorporation of external (to the ICR cell) multipole devices with FTICR for ion selection and ion a

19 force field, was chosen as it includes both multipole electrostatics and polarizability thought to b

20 The polarizable atomic multipole electrostatics model implemented in the AMOEBA

21 hod allows for the measurement of local high-multipole excitations and is bulk-sensitive.

22 the model-independent approach based on the multipole expansion method to provide a stable and uniqu

23 We present a multipole expansion that covers a large family of locali

24 e model describing spectroscopy includes the multipole-field interaction, which leads to established

25 icant advantages over spectroscopy using the multipole-field interaction: flexible transition rules a

26 y was modeled with use of the Hansen-Coppens multipole formalism, and features associated with both i

27 haracterisation of the flow and transfers in multipole Hele-Shaw configurations.

28 collisional activation, similarly to RF-only multipole ion guides and traps.

29 Radio frequency (RF) multipole ion guides that allow for collisional cooling

30 sight into the ion dynamics occurring inside multipole ion guides.

31 generated by a core dynamo, but higher order multipoles may be important as they are at Uranus and Ne

32 bspace methods and a new version of the fast multipole method.

33 The Hansen-Coppens multipole model as implemented in the XD program gave R

34 estrone crystal has been described with the multipole model, which allowed extensive topological ana

35 crystal was modeled using the Hansen-Coppens multipole model.

36 density was modeled using the Hansen-Coppens multipole model.

37 the methodology based on the exact potential multipole moment (EPMM) or classical molecular mechanics

38 ng structural unit that carries an ME-active multipole moment.

39 We extend this concept to higher electric multipole moments and determine the necessary conditions

40 Three types of such multipole moments are known: toroidal; monopole; and qua

41 significantly better than that obtained with multipole moments derived directly from the aspherical a

42 So far, however, the ME activity of these multipole moments has only been established experimental

43 Such multipole moments have broken space-inversion and time-r

44 ts highlight the importance of electrostatic multipole moments in determining aromatic-aromatic inter

45 onal change reveal that, with the side chain multipole moments intact (+MP), the EtF conformation is

46 ed by the magnitudes and orientations of the multipole moments of varying order.

47 Using high rank multipole moments we show that the atomic partitioning o

48 ts, multiple spins can combine into emergent multipole moments.

49 However, removing the electrostatic multipoles of the Trp side chains while retaining the di

50 ly and theoretically the lattice coupling of multipole plasmon modes for closely spaced gold nanorod

51 This lattice coupling of multipole plasmon modes is of broad interest not only fo

52 approach for accurate evaluation of dynamic multipole polarizabilities and van der Waals (vdW) coeff

53 Our theory predicts dynamic multipole polarizabilities in excellent agreement with m

54 orders from the electron density and static multipole polarizabilities of each atom or other spheric

55 ith ambient gas molecules in an intermediate multipole (q00) of the instrument.

56 We recently developed a polarizable atomic multipole refinement method assisted by the AMOEBA force

57 -C(5)H(5))(2)Fe(2) (4) have been obtained by multipole refinement of high-resolution X-ray diffractio

58 wavelength were analyzed theoretically using multipole scattering theory, where the complex refractiv

59 Using a multipole shielding polarizability-local reaction field

60 Multipole solutions yield non-dipolar contributions of 2

61 An alternative approach of multipole-storage-assisted dissociation (MSAD) has previ

62 ng collisional fragmentation in the external multipole that is usually employed for ion accumulation.

63 In contrast to conventional multipoles, the toroidal dipole interaction strength dep

64 Focusing on the three lowest-order multipoles-the total charge, dipole, and quadrupole mome

65 ctromagnetic interactions involving toroidal multipoles, which could be present in naturally occurrin

66 ables fabrication of nonlinear optical (NLO) multipoles with extraordinary hyperpolarizabilities.