| ²é¿´: 2707 | »Ø¸´: 3 | |||||||||||||||||
k_nowľ³æ (ÕýʽдÊÖ)
|
[½»Á÷]
¼¸¸öѧϰµÚÒ»ÐÔÔÀí¶¯Á¦Ñ§µÄÖØÒªÍøÖ· ÒÑÓÐ1È˲ÎÓë
|
|
1. NIC Series£º http://www.fz-juelich.de/nic-series/index.html (1)2006Äê NIC series V31: Computational Nanoscience: do it yourself ÊÇѧϰµÚÒ»ÐÔÔÀí¶¯Á¦Ñ§Ä£ÄâµÄÆðµã£» (2) 2000ÄêNIC Series Volume 1: Modern Methods and Algorithms of Quantum Chemistry Proceedings 2.Institute of Physical Chemistry@Univerity of ZurichµÄ×ÊÔ´ÏÂÔØ£ºhhttp://www.pci.uzh.ch/e/download.html 3.CECAM£ºhttp://www.cecam.org/ CECAM (Centre Europ¨¦en de Calcul Atomique et Mol¨¦culaire)ÊÇÒ»¸öÅ·ÖÞµÄ×éÖ¯£¬ÖÂÁ¦Óڸ߼¶¼ÆËã·½·¨µÄ»ù´¡Ñо¿ºÍÔÚÇ°ÑØ¿Æ¼¼ÁìÓòµÄÖØÒªÎÊÌâÉϵÄÓ¦ÓᣠAqueous Solvation of IonsLocation : CECAM-ETHZ, Zurich, Switzerland February 22, 2010 - February 24, 2010 van der Waals forces in DFT, RPA and beyondLocation : CECAM-HQ-EPFL, Lausanne, Switzerland June 28, 2010 - July 2, 2010 Modeling and Simulation of Water at Interfaces from Ambient to Supercooled Conditions.Location : CECAM-HQ-EPFL, Lausanne, Switzerland June 29, 2009 - July 1, 2009 Progress in ab initio modelling of biomolecules : towards computational spectroscopy Location : Dipartimento di Fisica Universit¨¤ di Roma April 2, 2007 - April 4, 2007 Vibrational spectroscopy of small molecules of biological interest in liquid water by Car-Parrinello simulations Rodolphe Vuilleumier Ecole Normale Sup¨¦rieure, Paris Abstract Vibrational spectroscopy, infrared or Raman, allows to get structural and dynamical informations about molecules in gaseous and aqueous phases. Ab initio Molecular dynamics simulations was proven to be able to reproduce the experimentally observed spectra in a variety of situations but their interpretation from the simulation is still a challenge. Here, we present an original method for analysing vibrational spectra from ab initio molecular dynamics at finite temperature, that generalizes normal modes to anharmonic systems. With the aid of these effective vibrational modes we can then determine the intensities and the widths of each infrared absorption bands allowing for an interpretation of the predicted signal. This method will be illustrated with the study of the infrared spectrum of N-methylacetamide, a model of the peptide bond, in gas phase and in aqueous solution, and of the vibrational spectrum of small peptides in gas phase. Hydrogen bonds, cooperativity, and the stability of helical polypeptides: towards a spectroscopic fingerprint Volker Blum Fritz Haber Institute, Berlin Abstract Hydrogen bonds are the basic stabilizing ingredient in many secondary structure elements of peptides and proteins. In finite polypeptide chains, simple estimates show that the strength of H bonds depends strongly on the length and environment of the peptide: e.g., the energy of a single isolated H bond in a short alpha-helical polypeptide is actually smaller by approximately a factor of two than the same energy for the H bonds of an infinite bulk-like alpha helix with the exact same H bond geometry. This effect is known as cooperativity of H bonds. We here use the new all-electron / full-potential, numeric atom-centered orbital based code package "FHI-aims" [1] ("Ab Initio Molecular Simulations" and the PBE generalized-gradient density functional to study the development of H bond cooperativity with chain length n for helical Polyalanine polypeptides(Ala)_n, for different helix types (3_10, alpha, pi) and termination (neutral or capped by positive alkali ions). For neutrally terminated helices (not experimentally stable in the gas phase), the increase of H bond strength is rather gradual with length. In contrast, an alkali ion termination (stable helices observed in gas phase experiments) stabilizes finite helices both directly, by saturating "dangling" terminating H bonds, and indirectly, by strengthening the remaining H bonds in a short helical chain, compared to the neutral case. It is a challenge to link these fundamental observations to experiment, by identifying a fingerprint of this cooperativity in the electronic structure of experimentally accessible short gas phase peptides. Besides the ground state electronic structure, this requires the proper description of at least the single (quasi-)particle spectra. We emphasize the importance of quasiparticle effects when comparing the calculated electronic structure with photoemission, and discuss the basic concepts of how many-body perturbation theory in the GW approach can be employed in the numeric atom-centered orbital based framework. Key References [1] V. Blum, R. Gehrke, P. Havu, V. Havu, X. Ren, M. Scheffler, The FHI Ab Initio Molecular Simulations (aims) Project, Fritz-Haber-Institut, Berlin (2007). ÔÍøÖ·£ºhttp://hi.baidu.com/xijunw/item/295cb9d3b3d040e6b2f777f4 [ À´×Ô¿ÆÑмÒ×å ¼Åį´ó³æ¼Ò×å ] |
» ÊÕ¼±¾ÌûµÄÌÔÌûר¼ÍƼö
¿ÆÑеç×ÓÊé¹²Ïí | µÚÒ»ÐÔÔÀí | SCIÊÕ¼ | ¿ÆÑм¼ÇÉ |
×ÊÔ´ | ÎïÀíÇ°ÑØ | ¼ÆËãÄ£Äâ-MS-CASTEP | ÄÉÃײÄÁÏ£¨MECHANISM) |
¼ÆËã·ÂÕæ | Á¿×Ó»¯Ñ§¼ÆËãÓëʹÓþÑé | ÔÓÆßÔÓ°Ë | ¼¤¹âÆ÷Èí¼þÄ£Äâ |
xuexijisuan | ¹ÌÌåÀíÂÛÓëµÚÒ»ÐÔÔÀí |
» ±¾ÌûÒÑ»ñµÃµÄºì»¨£¨×îÐÂ10¶ä£©
» ²ÂÄãϲ»¶
£¨µ÷¼Á£©Ò»Ö¾Ô¸±¨¿¼¹þ¶û±õ¹¤Òµ´óѧ0857×ÊÔ´Óë»·¾³×¨Òµ378·Ö¿¼Éú
ÒѾÓÐ6È˻ظ´
262Çóµ÷¼Á
ÒѾÓÐ7È˻ظ´
²ÄÁÏר˶322·Ö
ÒѾÓÐ10È˻ظ´
²ÄÁϵ÷¼Á
ÒѾÓÐ8È˻ظ´
085600£¬320·ÖÇóµ÷¼Á
ÒѾÓÐ8È˻ظ´
Ò»Ö¾Ô¸ ½ÄÏ´óѧ 085602 »¯¹¤×¨Ë¶ 338·ÖÇóµ÷¼Á
ÒѾÓÐ11È˻ظ´
Çóµ÷¼Á
ÒѾÓÐ6È˻ظ´
086000µ÷¼Á
ÒѾÓÐ3È˻ظ´
Çóµ÷¼Á
ÒѾÓÐ4È˻ظ´
0703µ÷¼Á£¬Ò»Ö¾Ô¸Ìì½ò´óѧ319·Ö
ÒѾÓÐ4È˻ظ´
» ±¾Ö÷ÌâÏà¹Ø¼ÛÖµÌùÍÆ¼ö£¬¶ÔÄúͬÑùÓаïÖú:
¿ªÊ¼µÚÒ»ÐÔÔÀíÈëÃÅѧϰ£¬ÏÈ·ÖÏíÏÂÈí¼þ¼°°²×°°É
ÒѾÓÐ8È˻ظ´
µÚÒ»ÐÔÔÀí·Ö×Ó¶¯Á¦Ñ§Ë㻯ѧ·´Ó¦£¨JACS£¬2012£©
ÒѾÓÐ47È˻ظ´
µÚÒ»ÐÔÔÀí·Ö×Ó¶¯Á¦Ñ§ÔËÓÃÈÈÁ¦Ñ§»ý·ÖÇó·Çг×ÔÓÉÄÜ
ÒѾÓÐ9È˻ظ´
µÚÒ»ÐÔÔÀíºÍ·Ö×Ó¶¯Á¦Ñ§µÄ¹ØÏµ£¿
ÒѾÓÐ8È˻ظ´
±¯´ßµÄµÚÒ»ÐÔÔÀí·Ö×Ó¶¯Á¦Ñ§Ä£Äâ
ÒѾÓÐ30È˻ظ´
¹ØÓÚµÚÒ»ÐÔÔÀíºÍ·Ö×Ó¶¯Á¦Ñ§Ä£Ä⣬»¹ÓÐmsÈí¼þ
ÒѾÓÐ9È˻ظ´
¹ØÓÚÃÉÌØ¿¨Âå·½·¨
ÒѾÓÐ15È˻ظ´
µÚÒ»ÐÔÔÀíÈçºÎÃèÊö»¯Ñ§·´Ó¦¶¯Á¦Ñ§£¿
ÒѾÓÐ21È˻ظ´
ÎÄÏ×ѧϰ£ºµÚÒ»ÐÔÔÀí¼ÆËãºÏ³É°±·´Ó¦ËÙÂÊ£¨science,2005£©
ÒѾÓÐ7È˻ظ´
¡¾ÇóÖú¡¿µÚÒ»ÐÔÔÀíÈí¼þÄÜ×öNPTϵ×Ú·Ö×Ó¶¯Á¦Ñ§Ä£ÄâµÄÔ¼þÓÐÄÄЩ£¿
ÒѾÓÐ8È˻ظ´
¡¾ÇóÖú¡¿ÓÐÈËÓÃDmol3×ö¹ýµÚÒ»ÐÔÔÀí·Ö×Ó¶¯Á¦Ñ§Âð
ÒѾÓÐ9È˻ظ´
¡¾ÇóÖú³É¹¦¡¿ÇóÍÆ¼öµÚÒ»ÐÔÔÀí·Ö×Ó¶¯Á¦Ñ§µÄÊé¼®
ÒѾÓÐ6È˻ظ´
¡¾Ô´´¡¿vaspµÄ·Ö×Ó¶¯Á¦Ñ§Ä£Äâ
ÒѾÓÐ44È˻ظ´

yjr
Ìú¸Ëľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ¹ó±ö: 0.033
- ½ð±Ò: 7839.2
- É¢½ð: 47
- ºì»¨: 2
- Ìû×Ó: 401
- ÔÚÏß: 1188.8Сʱ
- ³æºÅ: 770005
- ×¢²á: 2009-05-14
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
2Â¥2013-03-27 19:38:17
0.8
![]() |
3Â¥2013-03-28 22:21:51
japical
ͳæ (СÓÐÃûÆø)
- Ó¦Öú: 1 (Ó×¶ùÔ°)
- ½ð±Ò: 2780
- É¢½ð: 10
- ºì»¨: 3
- Ìû×Ó: 280
- ÔÚÏß: 63.7Сʱ
- ³æºÅ: 869727
- ×¢²á: 2009-10-12
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ

4Â¥2013-05-28 10:47:27














and the PBE generalized-gradient density functional to study the development of H bond cooperativity with chain length n for helical Polyalanine polypeptides
»Ø¸´´ËÂ¥
japical
120