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1 magnitude larger than those observed in bulk liquid helium.
2 es in their three-dimensional environment of liquid helium.
3 result of unique cluster growth processes in liquid helium.
4 alized in superconductors, atomic gases, and liquid helium.
5 ous cavitation in liquid nitrogen and normal liquid helium.
6                   Atomic quantum gases(1,2), liquid helium(3,4) and electrons in quantum materials(5-
7 estigation of transport properties in normal liquid helium-3 and its topological superfluid phases pr
8 operties that are different from the quantum liquids helium-3 and helium-4.
9 elastic compressive strain up to 99% even in liquid helium (4 K), almost zero loss of resilience afte
10 of a R- roton (a particle-like excitation in liquid helium-4) is antiparallel to its velocity.
11 he two-fluid model(3,4) and observed in both liquid helium(5) and in ultracold atomic gases(6,7), is
12  quantum liquids -- such as superconductors, liquid helium and atom Bose-Einstein condensates -- that
13 e classical "rotating bucket" experiments of liquid helium and ultracold dilute gases provides the me
14 e two-dimensional system on the interface of liquid helium and vacuum.
15                        Molecules immersed in liquid helium are excellent probes of superfluidity.
16 ntum mechanical processes that take place in liquid helium at ultra-low temperatures.
17 c spins spontaneously align in a magnet, and liquid helium becomes superfluid.
18 specially in the case of liquid nitrogen- or liquid helium-cooled detectors) should be monitored.
19 mplexity, cost, and technical demands of the liquid-helium-cooled superconducting instruments require
20   Reported here is a study of the effects of liquid helium cooling on the fragmentation of ions forme
21 ly on the design and construction of a novel liquid helium cryostat that accommodates variable-sized
22 ttle system to transfer them in and out of a liquid-helium cryostat that houses a superresolution flu
23 compressibility measurements on electrons on liquid helium demonstrating the formation of an incompre
24 haracterized in the gas phase, was formed in liquid helium droplets and studied with infrared spectro
25 ow the measurement of physical parameters of liquid helium during the operation of a dilution refrige
26 ince the observation of frictionless flow in liquid helium II(1,2).
27 and that the rapid quenching provided by the liquid helium inhibits its rearrangement to the more sta
28                                         When liquid helium is cooled to below its phase transition at
29 ept proposed by Landau to explain superfluid liquid helium is the elementary excitation of quantum pa
30 enic levels above a micrometer-thick film of liquid helium, is proposed as an easily manipulated stro
31 bility behavior when temperature crosses the liquid helium lambda point.
32 he top plate is cooled by heat exchange with liquid helium maintained at 4.2 K.
33 e and cytosine) are cooled to 0.37 kelvin in liquid helium nanodroplets and oriented in a large dc el
34 re naturally realized in superfluids such as liquid helium or cold atomic clouds(5-8).
35                      In superfluids, such as liquid helium or ultracold gases, the corresponding quan
36  below liquid nitrogen temperatures, various liquid helium stages have been constructed but have prov
37 via laser-excited Shpol'skii spectrometry at liquid helium temperature (4.2 K) is reported.
38 iority pollutants are directly determined at liquid helium temperature (4.2 K) with the aid of a cryo
39 sibility field H*(T)-is approximately 7 T at liquid helium temperature (4.2 K), significantly lower t
40 of materials for SNSPD technology beyond the liquid helium temperature limit and suggests that even h
41 ifferent U isotopes ((238)U and (233)U), and liquid helium temperature time-resolved laser-induced fl
42 version imaging device, operating around the liquid helium temperature, based on the gallium arsenide
43 LLS is populated by thermal equilibration at liquid helium temperature.
44 ction at cryogenic temperatures (possibly at liquid helium temperatures and certainly above 75 K) imp
45                               EPR spectra at liquid helium temperatures and MCD spectra at room tempe
46 e(3+) signal is abolished by illumination at liquid helium temperatures and one whose Fe(3+) signal i
47 is quantum yield is temperature invariant at liquid helium temperatures and shows a rather large kine
48 channel silicon-on-insulator quantum dots at liquid helium temperatures by using a radio frequency (r
49 pin coherence is difficult to maintain above liquid helium temperatures due to typical crystal packin
50 uantized modes of a quantum point contact at liquid helium temperatures to be imaged.
51 ear double resonance (ENDOR) spectroscopy at liquid helium temperatures, the Cu(II) coordination geom
52                                           At liquid helium temperatures, the network exhibits another
53 ly attractive for high-field applications at liquid helium temperatures.
54 d the physical causes of information loss at liquid-helium temperatures, and overcome them using a co
55 (-1) and 10(4) cm(2) V(-1) s(-1) at room and liquid-helium temperatures, respectively, allowing the o
56         First, by imaging ballistic flows at liquid-helium temperatures, we observe a Landauer-Sharvi
57 , however, the QHE has been observed only at liquid-helium temperatures.
58 olid-phase compounds Cu(hfac)(2)L(R) at low (liquid helium) temperatures and approaches developed for
59 ets have raised their magnetic memories from liquid helium to liquid nitrogen temperature thanks to a
60              Here, we introduce an ultracold liquid helium transmission electron microscope side-entr
61 emingly remote physical systems ranging from liquid helium, ultracold atoms and superconducting thin
62 asts with previous experiments on superfluid liquid helium where hysteresis was observed directly in
63 -magnetic Dewar flask and the consumption of liquid helium, which restricts the variability of the se