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1 hich is difficult in high-energy physics and cosmology.
2 e between idea and discovery, as SDSS did in cosmology.
3 arch fields, ranging from fluid mechanics to cosmology.
4 physics models from quantum field theory to cosmology.
5 se, with implications to network science and cosmology.
6 the galactic halo according to the standard cosmology.
7 outstanding puzzles in particle physics and cosmology.
8 ntral tenet of the cold dark matter model in cosmology.
9 erent approach to the dark energy problem in cosmology.
10 ere is still a great deal left to explore in cosmology.
11 waves, the Lense-Thirring effect, and modern cosmology.
12 rse that engages today's burgeoning field of cosmology.
13 d to illustrate the fine-tuning mechanism in cosmology.
14 which remains one of the unsolved puzzles of cosmology.
15 lenge that drives the field of computational cosmology.
16 wined with ancestors myths from contemporary cosmology.
17 n be used to distinguish between alternative cosmologies.
20 f phenomena ranging from particle physics to cosmology and from astrophysics to quantum chemistry.
22 Universe remains one of the prime puzzles of cosmology and particle physics today-80 y after the firs
23 tter problem is now a pressing issue in both cosmology and particle physics, and the detection of par
25 ssential foundation of the standard model of cosmology and underlies our description of the black hol
26 many-body systems spanning condensed matter, cosmology, and beyond are hypothesized to be universal w
27 cting textures drawn from materials science, cosmology, and granular media, among other examples.
28 enetics, biochemistry, statistics, biometry, cosmology, and philosophy, although he himself possessed
29 tructure; summarize its impact on astronomy, cosmology, and physics; and look ahead by outlining the
31 termination of the fundamental parameters of cosmology, and to our understanding of both the past and
32 tandard siren approach of gravitational wave cosmology appeals to the direct luminosity distance esti
34 e to view the observational side of physical cosmology as a subdiscipline of astrophysics, still in a
35 tory of the Universe is a key goal of modern cosmology, as it is crucial to our understanding of how
36 ion enables tests of fundamental physics and cosmology, as well as practical applications such as sat
37 the IRAS galaxy samples by generic big bang cosmology (BBC) and chronometric cosmology (CC), respect
39 r historical example shows how a subfield of cosmology, big bang nucleosynthesis, grew in complexity
40 so its abundance is of interest not only for cosmology, but also for understanding stellar evolution
45 m provides support for the standard model of cosmology, in which dark matter and dark energy are the
49 for the dark matter (DM) of the hot big bang cosmology is about as good as it gets in natural science
50 volution hypothesis in the frame of big-bang cosmology is confirmed at a high level of statistical si
51 ure radiation phase of the Standard Model of Cosmology is embedded as a single point in this family.
57 One of the key questions in observational cosmology is the identification of the sources responsib
60 Although general relativity underlies modern cosmology, its applicability on cosmological length scal
61 past 20 years have seen dramatic advances in cosmology, mostly driven by observations from new telesc
62 0, Lambda = 0 denoted as C1 and chronometric cosmology (no relevant adjustable parameters) denoted as
66 nature, appearing in contexts as diverse as cosmology, particle physics, superfluidity, liquid cryst
67 ions for tests of unification models and for cosmology (source counts, measurements of the Hubble con
69 rameters (in contrast to the two in big-bang cosmology), the hypothesized evolution appears from the
71 nt as dark matter is in our understanding of cosmology, the detection of these particles has thus far
72 e computational systems originally built for cosmology, the Sloan Digital Sky Survey (SDSS), are now
73 ns that the three fundamental observables in cosmology-the age of the Universe, the distance-redshift
74 er effect is out of the mainstream of modern cosmology, this article opened the way to investigation
76 of phase transitions in systems ranging from cosmology to condensed matter and quantum materials.
79 oincides with the prediction of chronometric cosmology, which estimates R as 160 +/- 40 Mpc (1 parsec
80 odel as represented by the Friedman-Lemaitre cosmology with parameters qo = 0, Lambda = 0 denoted as
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