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10/7 ¤ÇÆüµ­³«»Ï¤«¤é°ìǯ·Ð¤Ã¤Æ¤¤¤¿¡£ »Ò¶¡¤Î¤³¤í¤Ë²¿²ó¤«Æüµ­¤ò¤Ä¤±¤«¤±¤¿¤³¤È¤Ï¤¢¤ë¤±¤É¡¢ ¿ô¥ö·î¤¹¤é»ý¤Ã¤¿»î¤·¤¬¤Ê¤«¤Ã¤¿¤Î¤À¤¬¡£ ¤¢¤ê¤¬¤¿¤ä > hns

#2 [freshmeat] 10/1¡Á10/8 ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#3 [LDP] ¡Á10/8 ¤Î updates

#4 [URL] Translation Memory Systems

For technical communicators exploring translation services, a relatively new technology can help provide consistency among translated documents, make the translation process more efficient, and make translation projects cost effective. Translation memory systems assist human translators by following along as a document is translated, creating a database of translated material and terminology, and allowing translators to access previously translated material easily. Using this technology, translators can translate, save, and reuse material, making the resulting translations highly consistent and the overall process more efficient and cost effective than working without this technology.
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#5 [LDP] ldp-discuss ¤«¤é

Merrill ¤µ¤ó¤Î¥³¥á¥ó¥È¡£¤É¤³¤Ç¤âÊú¤¨¤Æ¤¤¤ëÌäÂê¤Ï»÷¤Æ¤¤¤ë¡©
I am stepping up to volunteer to take on some more responsibilities for
the LDP. I am going to try to manage the document base. Here are the
things I am going to try to do:

1. Keep track of things like file formats, licenses, versions,
meta-data, and indexing.

2. Compile metrics on the documents, such as accuracy, completeness,
readability, etc., and identify problem areas.

3. Build a documentation "map" so we know what documentation we might
want to seek out in the future. We could post these on the TODO list.

4. Establish procedures for document provenance, which we completely
lack right now.

5. I am thinking about how we might institute a periodic review process,
so that each document is looked at by a volunteer and those that need
updating are identified.

6. I'm open to suggestions from anyone on what other activities might
improve the overall quality of our collection.

#6 [URL][JF] docbook ¤ÎËÝÌõÊýË¡

shom ¤µ¤ó¤Ë¶µ¤¨¤Æ¤¤¤¿¤À¤¯¡£rpm ·Ï¤Ç¤Î´Ä¶­¹½Ãۤ⤳¤ì¤Ç¤ª¤Ã¤±¡¼¡©
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#5 [labo][URL] U of I Computational Optical and Discharge Physics Group

Univ. Illinois ¤Î¥µ¥¤¥È¡£¤¦¤¦¡¢¤¿¤¯¤µ¤óÆɤޤͤС£ Dr. ¤Î³ØÀ¸¤Î Lu ¤µ¤ó¤«¤é¥á¡¼¥ë¤Ç¶µ¤¨¤Æ¤â¤é¤¦¡£ ®¹¶¤Ç¤ªÊÖ»ö¤ò½Ð¤¹¡£ÃçÎɤ¯¤Ê¤ì¤ë¤È¤¤¤¤¤Ê¤¢¡£

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#1 [URL] Debian JP Project

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#1 [LDP] 10/12 ¤Î updates

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#2 [labo] Hall ¬ÄêÁõÃÖΩ¤Á¾å¤²

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#1 °ÍÅÄ̾¿ÍÃÂÀ¸

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#4 [freshmeat] 10/13 ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#5 [labo] ´¸¦À¸ÎعÖ

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#7 [linux] Re: EtherChip ¤Ë¤Ä¤¤¤Æ (Re: IPmasquerade ¤Ë¤Ä¤¤¤Æ)

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2000ǯ10·î14Æü(ÅÚ) [nǯÆüµ­]

#1 [LDP] 10/14 ¤Î update

#2 ÀîºêÀܹü±¡

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#3 [freshmeat] 10/14 ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

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#1 ºòÈÕ¡Áº£Ä«

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#2 [JM] LDP man-pages complete

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#5 [linux] [SECURITY] New version of nis released

#6 WinLPrt 6.03.7

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#7 [paper] APL 10,17,24,31 July & 7 August 2000

¤¦¤¦¡¢¤Þ¤¿Î¯¤á¤¿¡£No.5 ¤Ï¥Ò¥Ã¥È¤Ê¤·¡£

¡÷ APL 77(2) pp.190 (2000):

¥«¥ë¥³¥Ñ¥¤¥é¥¤¥È·¿¤Î I-III-VI2 ²½¹çʪ¡¢ Ag(Ga|In)(S|Se|Te)2 ¤Î¥Ð¥ó¥É·×»»¤È ¦Ö(2) ¸÷³Ø·¸¿ô¤ÎÂè°ì¸¶Íý·×»»¡£ LMTO-LDA¡£¤ä¤Ã¤Ñ¤ê½Å¤¤ In, Te ¤¬Æþ¤ë¤ÈÂ礭¤¯¤Ê¤Ã¤Æ¤¤¤ë¡£

¡÷ APL 77(2) pp.217 (2000):

ÅìËÌÂç¤Î¥°¥ë¡¼¥×¡£p ·¿ Si(100) ¾å¤Ë¥¬¥¹¥½¡¼¥¹ MBE ¤Ç Ge ¤òÂÏÀѤµ¤»¡¢¥Ý¥¹¥È¥¢¥Ë¡¼¥ë¤ÇȯÀ¸¤¹¤ë island density ¤ò AFM ´Ñ»¡¡£ Ge ¤Î¾å¤Ë Si ¤Î cap layer ¤ò¤Ä¤±¤ë¤È¡¢È¯À¸Ì©ÅÙ¤¬¾å¾º¤¹¤ë¡¢¤È¤¤¤¦·ë²Ì¡£ Si ¤ò¤Ä¤±¤ë¤È surface diffusion ¤¬ÍÞÀ©¤µ¤ì¡¢¹çÂΤ¬µ¯¤³¤ê¤Ë¤¯¤¯¤Ê¤ë¡¢ Si ¤È Ge ¤ÎÁê¸ß³È»¶¤Ë¤è¤Ã¤Æ³ËÀ¸À®¤Î energy barrier ¤¬Ä㤯¤Ê¤ë¡¢ ¤Ê¤É¤Î¿äÏÀ¡£

¡÷ APL 77(2) pp.259 (2000):

GaAs(001) ¾å¤ËÀ®Ä¹¤µ¤»¤¿ CuGaSe2 Ëì¤Î PPA (piezoelectric photoacoustic) ¬Äê¡£Èóȯ¸÷¤Î carrier recombination ¤ò´Ñ»¡¤Ç¤­¤ë¼êË¡¤È¤Î¤³¤È¡£ ºÆ·ë¹ç energy (¥Ð¥ó¥ÉÉý) ¤ËÂбþ¤¹¤ë 1.73, 1.83, 2.04 ¤È¤¤¤Ã¤¿ 3 ¤Ä¤Î¥Ô¡¼¥¯¤È¡¢ ¤½¤ì¤é¤Î²¹Åٰ͸À­¤ò¬Äê¡£

¡÷ APL 77(3) pp.343 (2000):

Cu ¤Î EAM »È¤Ã¤¿ MD ¤Ç¡¢¼´±þÎϲ¼¤Ë¤ª¤«¤ì¤¿ void ¤Î growth ¤òÄɤä¿Ïᣠscrew dislocation ¤«¤é¤Îγ»ÒÊü½Ð¤Ë¤è¤Ã¤Æ void ¤¬À®Ä¹¤·¡¢ strain ¤¬´ËϤµ¤ì¤ë¤Î¤Ç¤¢¤ë¡¢¤È¤Î¤³¤È¡£

¡÷ APL 77(3) pp.352 (2000):

Cu strip (0.5um Éý) ¤ò Scanned Laser Annealing¡¢ bumboo structure ¤ÎÀ®Ä¹¤ò¸«¤¿Ï᣷뾽¤ÎŤµ¤ÏÉý¤Î 10 ÇÜÄøÅ٤ޤǡ¢ ²¹ÅÙ·¹¼Ð¤¬µÞ·ã¤ÊÊý¤¬Ä¹¤¯¤Ç¤­¤ë¡¢¤Ê¤É¡£

¡÷ APL 77(3) pp.362 (2000):

Au poly Ëì¤Î AFM ¤Ë¤è¤ë nano indentation ¬Äê¡£ grain °ì¸Ä¤ò¸«¤Ä¤±¤Æ¤½¤Î¾å¤Ç¼Â¹Ô¡£ force curve ¤ÏľÀþ¡¢1nm ¤Î²¡¤·¹þ¤ß¤Ç 400¡Á600 nm ÄøÅÙ¡£ ´ðÈĤ¬ quartz, mica, sapphire ¤Î½ç¤Ë¸Ç¤¯¤Ê¤Ã¤Æ¤¤¤ë¡£ ÃͤȤ·¤Æ¤Ï 70¡Á90MPa ÄøÅÙ¡¢polycrystalline bulk ¤Î 1/3 ÄøÅÙ¤ÎÃͤǡ¢ ¤«¤Ä²¡¤·¹þ¤ß¥¨¥ê¥¢¤¬¾®¤µ¤¤¤È¾®¤µ¤¤¡£ ·ç´ÙÌ©ÅÙ¤¬¾®¤µ¤¤¤»¤¤¤À¤í¤¦¡¢¤Ê¤É¤ÎµÄÏÀ¡£

¡÷ APL 77(4) pp.489 (2000):

·ÄÂç¿¿ÊÉÀèÀ¸¤Î¥°¥ë¡¼¥×¡£Ê¿¹ÔÊ¿ÈÄÅŶˤÎÊÒ¤ÃÊý¤Ë 700kHz ¤Î¡¢ ¤â¤¦°ìÊý¤Ë 100MHz ¤ÎÅÅ°µ¤ò¤«¤±¡¢Ì©ÅÙ¤È bias ¤òξÊý¥³¥ó¥È¥í¡¼¥ë¤·¤è¤¦¤È¤¤¤¦»î¤ß¡£ OES ¤Ë¤è¤ë Ar Î嵯¾õÂÖ¤ÎÌ©ÅÙ¤ò¸«¤Æ¡¢ÅÅ°µÈ椬ȯ¸÷¤ÎÈóÂоÎÀ­¤ËÍ¿¤¨¤ë¸ú²Ì¤ò´Ñ»¡¡£ ¹â¼þÇÈÅŶ˦¤ÎÅÅ°µ¤¬¡¢¤½¤ì¤Û¤É OES ¤Ë±Æ¶Á¤òÍ¿¤¨¤º¤Ë self-bias ¤Ë¤Ï¤Á¤ã¤ó¤È¸ú¤¤¤Æ¤¤¤ë¤È¤Î¤³¤È¡£

¡÷ APL 77(4) pp.492 (2000):

°ìÍͤÊÂçÌÌÀѥץ饺¥Þ¤òÀ¸À®¤¹¤ë¤¿¤á¤Î¹â¼þÇÈ¥¢¥ó¥Æ¥Ê¤ÎÀ߷ס£ Ʊ¿´¾õ¤Ë turn coil ¤òʤ١¢°ìÈÖ³°Â¦¤Ë¤Ï²ÄÊÑ¥³¥ó¥Ç¥ó¥µ¤ò¤Ä¤Ê¤¤¤Ç¤¤¤ë¡£ ¥·¥ß¥å¥ì¡¼¥·¥ç¥ó¤ò¹Ô¤¤¡¢ LC ¤Î¶¦ÌĤ¬µ¯¤³¤ë¤¢¤¿¤ê¤Ç°ìÈÖ¤¤¤¤ radial plasma profile ¤¬ÆÀ¤é¤ì¤ë¤È¤Î¼çÄ¥¡£

¡÷ APL 77(4) pp.495 (2000):

C4F8/Ar ¥×¥é¥º¥Þ¤Ë¤ª¤±¤ëÉ饤¥ª¥óÌ©Å٤άÄê¡£ 266nm ¤Î YAG pulse ¤òÆþ¤ì¤Æ photodetachment ¤òµ¯¤³¤·¡¢ ¤½¤Î»þ¤ÎÅÅ»ÒÌ©ÅÙ¤ÎÊѲ½¤ò¥ß¥êÇÉ Fabry-Perot ¶¦¿¶´ï¤ò¤Ç´Ñ»¡¡£ 25mTorr ¤Î C4F8(5¡Á20%)/Ar ¥¬¥¹¤Ç¡¢¤ª¤è¤½ 10^11cm^-3 ÄøÅ٤Υ¤¥ª¥óÌ©Å٤Ȥ«¡£ electron attachment ¤Î rate eq. ¤«¤é·ë²Ì¤òɾ²Á¤·¤Æ¤¤¤ë¡£

¡÷ APL 77(6) pp.800 (2000):

Langmuir probe ¤Ë¤è¤ë»ÀÁǥץ饺¥ÞÃæ¤ÎÅŻҡ¦ÀµÉ饤¥ª¥óÌ©ÅÙ¬Äê¡£ É饤¥ª¥ó¤Ï photo detachment ¤È "double peak" methoc (ref 10) ¤«¤é·èÄê¡£ 3¡Á30Pa, radial profile¡£FMT ¤È¤¤¤¦¡¢¤³¤Î¥°¥ë¡¼¥×¤¬³«È¯¤·¤¿·×»»¥â¥Ç¥ë¤ÈÈæ³Ó¡£ °µÎϤ¬¾å¤¬¤ë¤È¤¢¤Þ¤ê°ìÃפÏÎɤ¯¤Ê¤¯¤Ê¤Ã¤Æ¤¤¤ë¡£ É饤¥ª¥óÌ©ÅÙ¤ÎÂ礭¤µ¤Ï¤À¤¤¤¿¤¤ 10^15 m^-3 ÄøÅÙ¡£

¡÷ APL 77(6) pp.839 (2000):

MgO (100) ¤Î nanoindentation¡£ 10nm ÄøÅ٤ޤǤΠforce curve ¤Ë¤ª¤¤¤Æ¡¢ÁºÀ­Îΰè¤Ç¤Ï force °ìÄê¤Ç ¥º¥Ö¥º¥ÖÆþ¤Ã¤Æ¤¤¤¯¤è¤¦¤ÊÎΰ褬¤¢¤ê¡¢¸¶»ÒÁؤËÂбþ¤·¤Æ¤¤¤ë¤Î¤Ç¤Ï¡¢¤È¤Î¤³¤È¡£ ¤½¤ÎÁ°¤Î Hrtzizn ¤ÊÎΰè¤Ç¤Î reduced Young's modulus ¤Ï 100GPa ¤¯¤é¤¤¡£
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2000ǯ10·î16Æü(·î) [nǯÆüµ­]

#1 [URL] Á´¹ñ¤ª½É¾ðÊó¡Ö¤ä¤ÉÂÀϺ¡×

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#2 [URL] Voice-Trek VT1000RV

¤¤¤Ä¤Ç¤â¡¢¤É¤³¤Ç¤â´Êñ¤ËÏ¿²»¤¬¤Ç¤­¡¢ Ï¿²»¤·¤¿²»À¼¤ò¥¹¥Ô¡¼¥Ç¥£¡¼¤Ëʸ»úÊÑ´¹¤Ç¤­¤ë¥â¥Ð¥¤¥ë²»À¼Ê¸»úÊÑ´¹¥·¥¹¥Æ¥à Voice-Trek VT1000RV ¡Ê¥Ç¥¸¥¿¥ë¥Ü¥¤¥¹¥ì¥³¡¼¥À¡¼£Ä£±£°£°£°¡ÜViaVoice Transcription with DSS Player¡ÊÃí¡Ë¡Ë¤òȯÇ䤤¤¿¤·¤Þ¤·¤¿¡£
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#3 [paper] PRL 24,31 July & 7 August 2000

¡÷ PRL 85(4) pp.780 (2000):

CaF2 ¤ò glancing angle ¤Ê 4.5keV Ar (200L) ¤Ç¥¹¥Ñ¥Ã¥¿¡¢ F ¤¬ preferenctial ¤ËÈ´¤±¤ë¤Î¤Ç¡¢»Ä¤Ã¤¿ Ca ¤¬ 2ML ÄøÅ٤Πbubble ¹½Â¤¤ò¤È¤ë¡¢¤È¤Î¤³¤È¡£ AFM ¤Ç´Ñ»¡¡£ lattice mismatch ¤¬ 2% ÄøÅÙ¤¢¤ë¤Î¤Ç tensile ¤Ê stress ¤¬È¯À¸¡¢ ¤½¤ì¤Ë¤è¤Ã¤Æ¥Ð¥Ö¥ë¹½Â¤¤ÎÆÃħŪ¤Ê¥¹¥±¡¼¥ë¤¬·è¤Þ¤ë¤Î¤À¡¢¤È¤ÎµÄÏÀ¡£

¡÷ PRL 85(4) pp.800 (2000):

Ag (100) ¤Î MBE ¤Ë¤è¤ë¥Û¥â¥¨¥Ô 25ML¡£ ´ðÈIJ¹ÅÙ¤ò 62¡Á300K ¤ÈÊѤ¨¤Æ STM ´Ñ»¡¡£ W ¤¬ 130K ÉÕ¶á¤Ç¶Ë¾®¡¢200K ÉÕ¶á¤Ç¶ËÂç¡¢¤½¤Î¸å¤Ï RT ¤Þ¤Ç¸º¾¯¡£ Ëì¤Ï 3d island ¾õ¤Î mound ¤«¤é¤Ê¤Ã¤Æ¤¤¤Æ¡¢island ´Öµ÷Î¥¤Ï²¹Å٤ȤȤâ¤ËñĴÁý²Ã¡£ ²¹Å٤ι⤤Êý¤«¤é¡¢interlayer diffusion ¤Î¸º¾¯¡¢Shwoebel barrier ¤Ë¤è¤ë terrace diffusion ¤ÎÍÞÀ©¡¢local ¤Ê nearest neibour ¤Î¿¤¤ site ¤Ø¤Î trap ¤Ë»ÙÇÛ¤µ¤ì¤ë self-affine like ¤ÊÀ®Ä¹¡¢¤¬¸ú¤¤¤Æ¤ë¤Î¤Ç¤Ï¤Ê¤¤¤«¡¢¤ÈµÄÏÀ¡£ »²¹Í¤Ë¤Ê¤ë¡£

¡÷ PRL 85(5) pp.1250 (2000):

cluster beam ¤Î melting point ¤Î¬Äê¡£ ¥Î¥º¥ë¤Î²¹ÅÙ¤òÊѤ¨¤Æ calorimetry ¤Ç·èÄê¡£ 430¸Ä¤Î Sn ¥¯¥é¥¹¥¿¤Ç¡¢TM¡Á380K, 40meV/atom ÄøÅÙ¤ÎÍ»²òenergy¡£ bulk ¤À¤È 505K, 73meV¡£¥µ¥¤¥º°Í¸À­¤â¬¤ê¡¢ ɽÌ̤Πpremelt ¤¬¸ú¤¤¤Æ¤¤¤ë¤Î¤Ç¤Ï¡¢¤È¤ÎµÄÏÀ¡£

¡÷ PRL 85(6) pp.1000 (2000):

metal tip - insulater substrate ´Ö¤Î stick-slip friction ¤Ç¡¢ ´ðÈĤËÃßÀѤµ¤ì¤ë charge ¤Î±Õ¾½¤Ë¤è¤ë imaging ¤È AC chopper ¤Ä¤«¤Ã¤¿ ÀäÂЬÄê¡£slip size ¤È charge ¤ÏÀþ·Á´Ø·¸¤¬¤¢¤ê¡¢ stick-slip motion ¤Ë¤ÏÅŲ٤αƶÁ¤¬Â礭¤¤¡¢¤È¤Î·ëÏÀ¡£

#4 [paper] next year subscription

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#1 [LDP] 10/17 ¤Î updates

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#3 [labo] »³ËÜ¿¿¶õ¤Î¿¿¶õ·×¥³¥ó¥È¥í¡¼¥é

ºòÆü fax ¤ÇÌä¹ç¤ï¤»¤¿·ï¡¢¥¨¥ß¥Ã¥·¥ç¥ó¤¬¾å¤¬¤é¤Ê¤¤¥È¥é¥Ö¥ë¤À¤í¤¦¡¢¤È¤ÎÊÖ»ö¡£ µå¤ÏÀÚ¤ì¤Æ¤Ê¤¤¤è¤¦¤Ë¸«¤¨¤ë¤Î¤À¤¬¡£ ÂÎÄ´¤¬Ìá¤Ã¤¿¤é¡¢Ê̤Υ³¥ó¥È¥í¡¼¥é¤Ç¥Á¥§¥Ã¥¯¤Î¾å¡¢ ¤¤¤«¤ì¤Æ¤¿¤é½¤Íý°ÍÍê¡¢¤«¤Ê¡£

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#5 [URL] pointer home

linux-users ML ¤ÇÌîß·¤µ¤ó¤¬¾Ò²ð¡£
pointer ¤È¤Ï UNIX¡Ê¤È¸Æ¤Ð¤ì¤ë OS¡Ë¾å¤Ç X-window ¤òÍѤ¤¤¿¡¢ x-y ¤Î¥Ç¡¼¥¿¤«¤é¥°¥é¥Õ¤òÉÁ²è¤µ¤»¤ë¤¿¤á ¤Î¥½¥Õ¥È¥¦¥¨¥¢¤Ç¤¹¡£ ƱÍͤΥ½¥Õ¥È¥¦¥¨¥¢¤È¤·¤Æ¤¹¤Ç¤Ë 'lick mongo', 'gnuplot' ¤È¤¤¤Ã¤¿¤â¤Î¤¬Â¸ºß¤·¤Þ¤¹ ¤¬¡¢ pointer ¤Ï¡Ö¼ê·Ú¤µ¡×¤Ë½ÅÅÀ¤ò¤ª¤¤¤Æ¡¢ tcsh É÷¤Î¥¤¥ó¥¿¡¼¥Õ¥§¥¤¥¹¤ä shell-script¡¢perl Ū¤Ê ¥×¥í¥°¥é ¥à²½µ¡Ç½¤òºÎ¤êÆþ¤ì¤Æ¤¤¤Þ¤¹¡£ 1996 ǯ¤Ë ver 1.0 ¤¬´°À®¤·¤Þ¤·¤¿¤¬¡¢ 1998 ǯ¤Ëµ¡Ç½¤ò²þ¤á¤Æ¡¢ ¸½ºß ver 2.00 ¤Î¥Ù¡¼¥¿ÈǤޤǴ°À®¤·¤Æ ¤¤¤Þ¤¹¡£

#6 [URL] Python ¥¹¥¯¥ê¥×¥È¤òºÎÍѤ·¤¿¥Æ¥­¥¹¥È¥¨¥Ç¥£¥¿--¡ÖKaaEdit¡×v1.5.0

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#2 [URL] VT100.net: Terminal Information

This site is dedicated to the range of video terminals produced by Digital Equipment Corporation (DEC) from 1970 to 1995. The most famous of these is the VT100, a name which is recognised most often today as a setting in terminal emulation programs.

#3 [URL] Video Terminal and Terminal-Emulator Information

Welcome to my collection of information concerning character-cell video-display terminals, serial-line remote-graphics terminals, and software that emulates them.

#4 [freshmeat] 10/16-17 ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#5 [LDP] 10/18-19 ¤Î updates

10/18 ʬ 10/19 ʬ

#6 [paper] An Ideal Gas of Beads

from Physical Review Focus:
Violently shaking a box of breakfast cereal does not make the particles act exactly like molecules in an ideal gas, but there are similarities. According to the 23 October PRL there is a simple mathematical expression for the distribution of particle velocities in a shaken box of steel beads which--like the formula for gas molecules--depends only on the average speed of the particles and not on the density or details of the shaking. To model problems such as grain motion in silos, soil shifting in earthquakes, and dry foods mixing in processing plants, physicists studying granular materials want equations as simple and comprehensive as those for gases and fluid motion. The new results suggest that such a theory may be possible.

#7 [labo][URL] ²Ê¸¦Èñ¥Þ¥¯¥í

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#8 [URL] ¤¿¤Þ¤Æ¤Ð¤³

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#9 [paper] JMR 15(8) August 2000

¡÷ JMR 15(8) pp.1653 (2000):

Çö¤¤¥¬¥é¥¹¤ò¸ü¤¤¥¬¥é¥¹¤Ë¥¨¥Ý¥­¥·¤ÇÀÜÃå¡¢indentation ¤Ç radial crack ¤È cone crack ¤ÎȯÀ¸¤ò¸«¤¿Ïᣠ´ðÈĤÎÁÈÀ®¤ò¤¤¤í¤¤¤íÊѤ¨¤Æ¹Å¤µ¤Î°ã¤¦¤â¤Î¤òÍÑ°Õ¡£ cone crack ¤ÎȯÀ¸¤Ï´ðÈĤνÀ¤é¤«¤µ¤Ë¤Ï°Í¸¤·¤Ê¤«¤Ã¤¿¤¬¡¢ radial crack ¤Ï´ðÈĤ¬¸Ç¤¤¤ÈȯÀ¸¤·¤Ë¤¯¤¯¤Ê¤ë (critical load ¤¬¾å¤¬¤ë) ·ë²Ì¡£

¡÷ JMR 15(8) pp.1693 (2000):

gold film ¤Î nano indentation¡£´ðÈÄ¤Ï Si, Ãæ´ÖÁØ¤Ë Cr ¤Þ¤¿¤Ï Ti¡£ bending machine ¤Ç¼´±þÎϤò²Ã¤¨¡¢indentation ¤Î force curve ¤Ë Hertzian fit ¤·¤Æ elastic modulus ¤ò¬Äê¡£ as depo ¤À¤È tensile ¤Ç¾®¤µ¤¯¡¢compressive ¤ÇÂ礭¤¯¤Ê¤ë·ë²Ì¤¬¡¢ aneeal ¤¹¤ë¤ÈµÕ¤Î·¹¸þ¤Ë¡£ indentor ¤Î¶ÊΨȾ·Â¤ËÂФ¹¤ë°Í¸À­¤Ç¤Ï¡¢R ¤¬¾®¤µ¤¤¤È¸Ç¤¯¸«¤¨¤ë¡£

¡÷ JMR 15(8) pp.1709 (2000):

¥¹¥Ñ¥Ã¥¿¤Ç SiO2 ¾å¤Ë¤Ä¤±¤¿ Al ¤Î hilock formation ¤Î´Ñ»¡¡£ ÉÔ½ãʪ¤È¤·¤Æ O, Ti, W ¤Ê¤É¤òƳÆþ¡£ H2/N2 ¥¬¥¹Ãæ¤Ç 2h 450¡î ¥¢¥Ë¡¼¥ë¤¹¤ë¤È¡¢island ¾õ¤Ë hilock ¤¬È¯À¸¡£ ³ä¤Ã¤ÆÃÇÌÌ TEM ¤È¤ë¤È¡¢hilock ¤Î²¼¤Ï Al ¤¬Ëä¤á¤Æ¤¤¤¿¡£ ¹â²¹¤ÇȯÀ¸¤·¤¿ void ¤Ë Al ¸¶»Ò¤¬ creep ¤·¤Æ¤­¤¿¤Î¤Ç¤Ï¤Ê¤¤¤«¡¢¤ÈµÄÏÀ¤·¤Æ¤¤¤ë¡£ hilock À¸À®¤Î¥â¥Ç¥ë¤È¤½¤Î·×»»Îã¤â¤¢¤ë¡£

¡÷ JMR 15(8) pp.1786 (2000):

microindentation ¤Î¥â¥Ç¥ë¡¦ÍýÏÀ·×»»¡£ dislocatoin ȯÀ¸¤¬ hardness ¤ò»ÙÇÛ¤¹¤ë micro scale ¤È¡¢ plasticity theory ¤Çµ­½Ò¤Ç¤­¤ë meso scale ¤òÀܳ¤¹¤ëÄê¼°²½¤È¤·¤Æ MSG (mechanism-based strain gradient) plastisity model ¤È¤¤¤¦¤Î¤¬¤¢¤ë¤½¤¦¤Ç¡¢ ¤½¤ì¤ò»È¤Ã¤Æ poly-Cu, (111) single-crystal Cu ¤Î depth-dependent hardness ¤ò ·×»»¡¢¼Â¸³¤È¤ÎÎɹ¥¤Ê°ìÃפò¸«¤Æ¤¤¤ë¡£

#10 [paper] JJAP part1 39(9A,9B) September 2000

9B ¤ÏͶÅÅÂκàÎÁ¤Î conference ¤Î proceedings.

¡÷ JJAP part1 39(9A) pp.5263 (2000):

XeCl ¥ì¡¼¥¶¤òÍѤ¤¤¿ laser abration ¤Î OES ´Ñ»¡¡£ Functionally Graded Materials ¤òºî¤ë¤¿¤á¤Ë±¾¡¹¡¢¤È¤¤¤¦Á°¤Õ¤ê¤¬Ä¹¤¤³ä¤ê¤Ë¤Ï¡¢ ¬¤Ã¤Æ¤¤¤ë¤Î¤ÏÅŻҲ¹ÅÙ¤À¤±¤È¤¤¤¦Ææ¤ÎÏÀʸ(¾Ð)¡£ Fe, Si, Al ¤Ê¤É¤Îȯ¸÷Àþ¤Î table ¤ÏÌò¤ËΩ¤Ä¤«¤â¡£

¡÷ JJAP part1 39(9B) pp.5369 (2000):

BaTiO3 ¤Î¥¹¥Ñ¥Ã¥¿¾øÃå¡£°µÎϤ¬Ä㤤¤È Ba/Ti <0.9 ¤À¤¬ 6Pa °Ê¾å¤Ë¤¹¤ë¤È stoichiometric ¤Ë¤Ê¤ë¤È¤«¡£¤¢¤È erosion track ¤«¤é¤Î³ÑÅÙ¤ËÂФ¹¤ë°Í¸À­¤â¡£ ¤¦¡¼¤ó¡¢Ti ¤ÎÊý¤¬·Ú¤¤¤ó¤À¤¬¤Ê¤¢¡£

¡÷ JJAP part1 39(9B) pp.5379 (2000):

¤³¤Á¤é¤Ï SrTiO3 ¤È SrRuO3¡£ Á°¼Ô¤Î¾ì¹ç¡¢ T-S µ÷Î¥¤òÎ¥¤¹¤È¡¢Ãæ´Ö¤Ç Ti ¤¬Â¿¤¯¤Ê¤ëÎΰ褬¡£ ¸å¼Ô¤ÏÃæ´Ö¤Ë Sr ¤Î¾®¤µ¤¯¤Ê¤ëÎΰ褬¡£ Êü½Ð³Ñ¤ÇÀâÌÀ¤·¤è¤¦¤È¤·¤Æ¤¤¤ë¤¬¡¢¤Á¤ç¤Ã¤È̵Íý¤¬¤¢¤ë¤Î¤Ç¤Ï...

#11 [linux] Photo Image Printing System for Linux

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#12 [paper] JJAP part2 39(9A/B,10A) 15 Septempber, 1 October 2000

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¡÷ JJAP part2 39(9A/B) pp.L908 (2000):

Cu/CaF2/Diamond ¤Ê MISFET ¤ÎºîÀ®Ë¡¤ÈÆÃÀ­É¾²Á¡£ CaF2 ¤À¤È interface state ¤¬Áý¤¨¤Ê¤¤¤Î¤Ç¤¤¤¤¤é¤·¤¤¡£
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#1 [LDP] 10/20 ¤Î updates

#2 [paper] PRL 85(7,8) 14,21 August 2000

¡÷ PRL 85(7) pp.1480 (2000):

Ag/Ag(111) ¾å¤Ç¤Î Schwoebel barrier ¤Ë´Ø¤¹¤ëÏÀʸ¡£ barrier heighte energy ¤Ï 0.13eV ¤ÈÊó¹ð¤µ¤ì¤Æ¤¤¤ë¤¬¡¢ prefactor ¤ÎÊý¤â·è¤á¤è¤¦¡¢¤È¤¤¤¦¤ªÏᣠRHEED ¤Î·ë²Ì¤ò Monte Carlo ¥â¥Ç¥ë¤ÈÈæ³Ó¤·¤¿¤È¤³¤í¡¢ simulation ¤Î¶¯ÅÙ decay ¤¬Â礭¤¯½Ð¤Æ¤·¤Þ¤Ã¤¿¡¢ ¤³¤ì¤Ï atom hopping ¤Î prefactor ¤Î¤»¤¤¤À¤í¤¦... ¤È¤¤¤¦¤³¤È¤Ç¡¢¥Æ¥é¥¹¾å¤Î prefactor ¤è¤ê step ¤Î prefactor ¤¬ 100 Çܤ¯¤é¤¤Â礭¤¤¡¢¤È¤Î·ë²Ì¡£ ¤³¤¤¤Ä¤¬²¹Åٰ͸À­¤ò¤Á¤ã¤ó¤ÈÀâÌÀ¤¹¤ë¤«¤É¤¦¤«¡¢¤¬¼¡¤Î²ÝÂ꤫¤·¤é¤ó¡£

¡÷ PRL 85(8) pp.1606 (2000):

nonequilibrium ¤Ê Hamiltonian system ¤¬ eq. ¤ËÊѲ½¤·¤Æ¤¤¤¯¤È¤­¤Î entropy À¸À®¤ò phase space ʬ³ä¤Ë¤è¤Ã¤Æ·×»»¤·¤è¤¦¤È¤¤¤¦Ïᣠº£²ó¤Ï»þ´Ö°Í¸À­¤ò»ý¤Á¹þ¤ó¤Ç¤¤¤ë¤È¤Î¤³¤È¡£ ·ë²Ì¤È¤·¤Æ¡¢¥¨¥ó¥È¥í¥Ô¡¼À¸À®¤Ï phase space ¤Ç¤Î fractal ¹½Â¤¤Î exponential decay ¤Ë°Í¸¤¹¤ë¡¢Ê¬³ä¤ÎγÅ٤ˤϰ͸¤·¤Ê¤¤¡¢¤Ê¤É¤Î·ë²Ì¡£

#3 [paper] APL 77(7,8) 14,21 August 2000

¡÷ APL 77(7) pp. (2000):

AC-PDP ¥Ñ¥Í¥ë¤Îȯ¸÷¸úΨ¤ÎÅÅÎϰ͸À­¤òÄ´¤Ù¤¿Ïᣠ°ì¤Ä¤ÏÊüÅÅÅÅ°µ¤òÊѤ¨¤ëÊýË¡¡¢¤â¤¦°ì¤Ä¤Ï dielectiric layer ¤Î ¸ü¤µ¤òÊѤ¨¤Æ capacitance ¤òÊѤ¨¤ëÊýË¡¡£ Á°¼Ô¤Ç¤ÏÅÅÎÏÁý²Ã¤È¤È¤â¤Ë´Ë¤ä¤«¤Ë¸úΨ¤Ï¾å¾º¡¢ ¸å¼Ô¤Ç¤ÏÅÅÎÏÁý²Ã¤È¤È¤â¤Ë¤Ï¤Ã¤­¤ê¤·¤¿¸º¾¯¤¬¸«¤é¤ì¤¿¡£ ÅÅÎϤ¬ÅŻҤò²ÃÇ®¤¹¤ë¤«¥¤¥ª¥ó¤ò²ÃÇ®¤¹¤ë¤«¤Çȯ¸÷¸úΨ¤¬·è¤Þ¤Ã¤Æ¤¯¤ë¤¬¡¢ ¤½¤ÎÊÕ¤ê¤ò¥â¥Ç¥ë·×»»¤Çɾ²Á¡¢¼Â¸³·ë²Ì¤È°ìÃפ¹¤ë·¹¸þ¡£¸¶°ø¤Ï unclear.

¡÷ APL 77(7) pp.975 (2000):

Íý¸¦¡¦Å칩Â祰¥ë¡¼¥×¡£ ZnO/(Mg,ZnO) ¿ÁØÎ̻Ұæ¸Í¹½Â¤¤Ç blue shift ¤ò´Ñ»¡¡¢ 3.3¡Á3.6 eV ¤Î PL ȯ¸÷À©¸æ¤¬²Äǽ¤Ë¤Ê¤Ã¤¿¤È¤Î¤³¤È¡£

¡÷ APL 77(8) pp.1096 (2000):

¥°¥é¥Õ¥¡¥¤¥È¤Ë CF3+ ¤ò 100eV ¤Ç¤Ö¤Ä¤±¤ë¤È¡¢CF3- ¥¤¥ª¥ó¤¬À¸À®¤µ¤ì¤ë¤È¤Î¼Â¸³¡£ Ag ¤ä PFPE ¤Ê¤É¤Ç¤Ï F- ¤·¤«¤Ç¤Ê¤¤¡£¶¦ÌÄÃæÀ­²½¡¦ÅÅ»ÒÉÕÃå³ÎΨ¤¬ metal ¤ËÈæ¤Ù¤Æ ¾®¤µ¤¯¡¢excited neutral ¤¬ decay ¤¹¤ë¤¿¤á²õ¤ì¤Ê¤¤¡¢¤Ê¤É¤ÈµÄÏÀ¡£ ´ØÏ¢¤·¤ÆÆþ¼Í³Ñ°Í¸À­¤Î¼Â¸³¤â¡£

¡÷ APL 77(8) pp.1099 (2000):

PLD ¤Çºî¤Ã¤¿¡¢´°Á´Ï¢Â³¤Ç¤Ï¤Ê¤¤ Cu Ëì¤Î¡¢in situ ¤Ç¤ÎÆ©²áΨ¡¦Åŵ¤Äñ¹³Â¬Äê¡£ Laser pulse ¤Î energy, T-S distance ¤ËÂФ¹¤ë percolation thickness ¤Ê¤É¡£ ¥¨¥Í¥ë¥®¡¼¤¬¾®¤µ¤¤Êý¤¬Çö¤¤¤¦¤Á¤ËϢ³Ëì¤Ë¤Ê¤ë¡£

#4 [freshmeat] 10/19 newsletter ¤«¤é

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#2 [LDP] 5/24 ¤Î updates

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#4 [URL] DNS Security Slides

#5 [linux] Broken debconf!

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#12 [paper] from arXiv cond-mat

¡÷ Roughening of close-packed singular surfaces:

An upper bound to the roughening temperature of a close-packed singular surface, fcc Al (111), is obtained via free energy calculations based on thermodynamic integration using the embedded-atom interaction model. Roughening of Al (111) is predicted to occur at around 890 K, well below bulk melting (933 K), and it should therefore be observable, save for possible kinetic hindering.
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