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18篇 您的检索式:作者名="Vorberg"
    题名 作者 年代 出处 被引量
1Molecular basis of scrapie strain glycoform variation显示文摘Vorberg I Priola S A 2002J Biol Chem2002,277,36:1
2Different time courses for visual perception and action priming显示文摘Vorberg D Mattler U Heinecke A Schmidt T & Schwarzbach J 0,,:1
3Molecular basis of scrapie strain glycoform variation显示文摘Vorberg I Priola SA 2002J Bio Chem2002,277,36:1
4Molecular basis of scrapie strain glycoform variation显示文摘 Priola S A 2002J Biol Chem2002,277,36:1
5Molecular basis of scrapie strain glycoform variation显示文摘Vorberg I Priola SA 2002J Bio Chem2002,277,36:1
6The time course of lexical access in speech production: A study of picture naming显示文摘Levelt WJM Schriefers H Vorberg D 1991Psychol Rev1991,98,:1
7Hydrogen-helium mixtures in the interiors of giant planets显示文摘Vorberger J Tamblyn I Militzer B 2007PhysRev B2007,75,02:1
8NA aptamers that bind to PrP(C) and not PrP(Sc)show sequence and structure specificity显示文摘Takemura K Wang P Vorberg I 2006Exp Biol Med (Maywood)2006,231,2:1
9Microstructure, oxidation resistance and high-temperature strength of ~, hardened Pt-base alloys显示文摘Wenderoth M Volkl R Vorberg S 2007Intermetallics2007,15,11:1
10Single-frequency operation of a diode-pumped lanthanum-neodymiumhexaaluminate laser by using a twisted-mode cavity显示文摘ADAMS C S VORBERG J MLYNEK J 1993Optics Letters1993,18,6:1
11DNA aptamers that bind to PrP(C)and not PrP(Sc)show sequence and structure specificity显示文摘TAKEMURA K WANG P VORBERG I 2006Exp Biol Med2006,231,2:1
12Microstructure, oxida- tion resistance and high-temperature strength of γ' hardened Pt-base alloys显示文摘Wenderoth M V61kl R Vorberg S 2007Intermetallics2007,15,:1
13The effects of Ta additions on the phase compositions and high temperature properties of Pt base alloys 显示文摘Rudnik Y Vorberg S 2008Materials Science and Engineering A2008,479,:1
14Microstructure, oxi- dation resistance and high temperature strength of rhardened Pt - base alloys显示文摘Wenderoth M Vorberg S Mitarai Y Y 2007Intemmtallics2007,15,:1
15The Time Course of Lexical Access in Speech Production:A Study of Picture Naming显示文摘Levelt W J M Schriefers H Vorberg D 1991Psychological Review1991,98,:1
16Hydrogen-helium mixtures in the interiors of giant planets显示文摘Vorberger J Tamblyn I Militzer B 2007Phys Rev B2007,75,02:1
17Therapy with garlic: results of a placebo-controlled, double-blind study显示文摘Vorberg G Schneider B 1990Br J Clin Pract Suppl1990,69,:1
18Physical insights from imaginary-time density–density correlation functions显示文摘An accurate theoretical description of the dynamic properties of correlated quantum many-body systems,such as the dynamic structure factor S(q,ω),is important in many fields.Unfortunately,highly accurate quantum Monte Carlo methods are usually restricted to the imaginary time domain,and the analytic continuation of the imaginary-time density–density correlation function F(q,τ)to real frequencies is a notoriously hard problem.Here,it is argued that often no such analytic continuation is required because by definition,F(q,τ)contains the same physical information as does S(q,ω),only represented unfamiliarly.Specifically,it is shown how one can directly extract key information such as the temperature or quasi-particle excitation energies from theτdomain,which is highly relevant for equation-of-state measurements of matter under extreme conditions[T.Dornheim et al.,Nat.Commun.13,7911(2022)].As a practical example,ab initio path-integral Monte Carlo results for the uniform electron gas(UEG)are considered,and it is shown that even nontrivial processes such as the roton feature of the UEG at low density[T.Dornheim et al.,Commun.Phys.5,304(2022)]are manifested straightforwardly in F(q,τ).A comprehensive overview is given of various useful properties of F(q,τ)and how it relates to the usual dynamic structure factor.In fact,working directly in theτdomain is advantageous for many reasons and opens up multiple avenues for future applications.Tobias Dornheim Zhandos A.Moldabekov Panagiotis Tolias Maximilian Böhme Jan Vorberger 2023Matter and Radiation at Extremes2023,8,5:0
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