¤Ê¤«¤Î¤Ë¤Ã¤­

ºÇ¿·ÈǤϤ³¤Á¤é¡£ Æͤùþ¤ß¤Ï³ÆÆüÉդΠBBS ¥¨¥ó¥È¥ê¤Î¤Û¤«¡¢ ¥á¡¼¥ë (nakano@st.seikei.ac.jp) ¤ä ¥Õ¥©¡¼¥à ¤«¤é¤É¤¦¤¾¡£ ¤Ê¤ª¥¹¥Ñ¥à½ü¤±¤Î¤¿¤á¡¢BBS µ¡Ç½¤Ë¤Ï ´Ë¤¤Ç§¾Ú¤òÆþ¤ì¤Æ ¤¤¤Þ¤¹¡£ ¸¡º÷¥¨¥ó¥¸¥ó¤«¤éÍ褿Êý¤Ï¡¢¥¨¥ó¥¸¥ó¤ÎÊý¤Î¥­¥ã¥Ã¥·¥å¤ò¸«¤ë¤«¡¢ ²¼¤Î´Ê°×¸¡º÷¤ò»î¤·¤Æ¤ß¤Æ¤¯¤À¤µ¤¤¡£


hns - Æüµ­¼«Æ°À¸À®¥·¥¹¥Æ¥à - Version 2.19.5

Àè·î 2001ǯ03·î Íè·î
Æü ·î ²Ð ¿å ÌÚ ¶â ÅÚ
1 2 3
4 5 6 7 8 9 10
11 12 13 14 15 16 17
18 19 20 21 22 23 24
25 26 27 28 29 30 31
Namazu for hns ¤Ë¤è¤ë´Ê°×Á´Ê¸¸¡º÷
¾Ü¤·¤¯¤Ï ¾ÜºÙ»ØÄê/¥Ø¥ë¥×¤ò»²¾È¤·¤Æ²¼¤µ¤¤
¸¡º÷¼°:

2001ǯ03·î21Æü(¿å) [nǯÆüµ­]

#1 [linux] sid ¤Î ssh ¤Î postinst ¥Ð¥°

¤¤¤Ä¤Þ¤Ç¤¿¤Ã¤Æ¤â¤Ê¤ª¤ëµ¤ÇÛ¤¬¤Ê¤¤¤Î¤Ç ¥Ñ¥Ã¥Á¤òÅꤲ¤Æ ¤ß¤ë¡£

¡÷ ¤È¤¤¤¦¤È¤³¤í¤Ç¼ê¸µ¤Ï¤Ê¤ª¤Ã¤¿¤¬:

/etc/init.d/ssh ¤â¤ª¤«¤·¤¤¤Ê... ¤Ê¤ó¤Ç /etc/ssh/NOSERVER ¤È /etc/ssh/sshd_not_to_be_run ¤ÈÆó¤Ä¤¢¤ë¤ó¤¸¤ã¡£ ¤È¤¤¤¦¤«¤½¤â¤½¤â¡¢rsh ¤ß¤¿¤¤¤Ë¥µ¡¼¥Ð¤È¥¯¥é¥¤¥¢¥ó¥Èʬ¤±¤ì¤Ð¤¤¤¤¤Î¤Ë¡£

¡÷ ¤·¤«¤·:

¤³¤Î BTS ¤ÎĹÂç¤Ê¥ê¥¹¥È¤ò¸«¤ë¤Ë¡¢ ¤³¤Î¥á¥ó¥Æ¥Ê¤Ï¥Ð¥°¤Î´ÉÍý¤¹¤ëµ¤¤¬¤Ê¤¤¤ó¤¸¤ã¤Ê¤¤¤Î¤«¡©

#2 [URL][linux] Linux ÍÑ¥×¥ê¥ó¥¿¥É¥é¥¤¥Ð

¥ê¥³¡¼¤Î¤Ï¡¢¤Á¤ç¤Ã¤È¤Þ¤È¤Þ¤Ã¤¿¥Ú¡¼¥¸¤Ï¸«¤Ä¤«¤é¤Ê¤«¤Ã¤¿¡£

#3 [LDP] 3/21 ¤Î updates

#4 [linux] sinonome ¥Õ¥©¥ó¥È¤È¹ç¤ï¤»¤ë iso8859 ¤Ê¥Õ¥©¥ó¥È

¼íÌ¤ó¤è¤ê Éí°¤·¤Æ¤¤¤ë ¤È¤Î¾ðÊó¤ò¤¤¤¿¤À¤¯¡£¤¹¤Ð¤é¤·¤¤¡£ ¤­¤Ã¤È gotom ÀèÀ¸¤¬ xfonts-shinonome ¤Ë merge ¤·¤Æ¤¯¤À¤µ¤ë¤Ë°ã¤¤¤Ê¤¤ :-)

¡÷ °ì­Àè¤Ë:

»î¤·¤Æ¤ß¤ë¡£krxvt ¾å vi ¤Ç .Xdefaults ¤òÀßÄêÃæ¤Î snapshot ¡£¤¤¤¤´¶¤¸¤Ç¤¹¤Í¤¨¡£

#5 [freshmeat] 3/20 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#6 [URL] Using Samba ¤ÎËÝÌõ¾õ¶·

°ìÄ̤êÌõ¤¬ÉÕ¤­¡¢ººÆÉ¥¹¥Æ¡¼¥¿¥¹¤ËÆþ¤Ã¤¿¤È¤Î¤³¤È¡£¤¹¤Ð¤é¤·¤¤¡£

¡÷ ¤Á¤ç¤Ã¤È¤º¤Ä:

¥Ñ¥Ã¥Á¤òÅꤲ¤Æ¤¤¤³¤¦¡£
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î22Æü(ÌÚ) [nǯÆüµ­]

#1 [URL] Free On-Line Dictionary Of Computing

ldp-discuss ¤Ç¾Ò²ð¤µ¤ì¤Æ¤¿¥³¥ó¥Ô¥å¡¼¥¿ÍѸì¸þ¤±¼­½ñ¥µ¥¤¥È¡£

Î㤨¤Ð "NUMA" ¤È°ú¤¤¤Æ¤ß¤ë ¤È¤³¤ó¤Ê´¶¤¸¡£
NUMA ==>
Non-Uniform Memory Access
<architecture> (NUMA) A memory architecture, used in multiprocessors, where the access time depends on the memory location. A processor can access its own local memory faster than non-local memory (memory which is local to another processor or shared between processors).
¾¤Ë¤Ï Glossary of the Linux FreeS/WAN project ¤Ê¤É¤â¡£

#2 ·ëº§¼°

Âç³Ø¤Î¥Ï¥ó¥ÉÉô¤ÎƱ´ü¤«¤é 5/19 ¤ËÈäϪ±ã¤ä¤ë¤È¤ÎÏ¢Íí¡£ ¤¦¡¼¤à¡¢¤³¤ì¤Ç»Ä¤ê¤Ï²¶¤À¤±¤Ë¤Ê¤Ã¤¿¤«¡¼(^^;

#3 [JM] bash.1 ¹»Àµ

½ªÎ»¡£ ¤Ò¡¼¡£

#4 [freshmeat] 3/21 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#5 [LDP] 3/22 ¤Î update

¤¤¤í¤¤¤í½Ð¤Þ¤¹¤Ê :-) »ÄÇ°¤Ê¤¬¤é xtt ¤ÎÏÃÂê¤Ï¾¯¤Ê¤¤¡£
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î23Æü(¶â) [nǯÆüµ­]

#1 Ææ¤Î¥á¡¼¥ë

Dear Sir
Hello
I don't know japan .
Will you help me?
I visited your site I want to get more information about gold karatage tester .
I want to buy one .
Please mail me the most information and catalog and its price.
spam ¤Ç¤Ï¤Ê¤¤¤è¤¦¤À¤¬... ¤Ê¤ó¤À¤³¤ê¤ã¡©

#2 ¥Î¥ÉÄË

°ì²óµÙ¤ß¡£¤°¤¦¡£

#3 [freshmeat] 2/23 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î24Æü(ÅÚ) [nǯÆüµ­]

#1 [LDP] 2/24 ¤Î updates

#2 [freshmeat] 3/23 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#3 MATRIX

WOWWOW ¤ÎÊüÁ÷¤Ç½é¤á¤Æ¸«¤¿(¾Ð)¡£¤ä¤Ã¤ÑÏÃÂê¤Ë¤Ê¤ë¤³¤È¤Ï¤¢¤ë¡£¤¹¤´¤¤¤Í¡£ DVD ¤Î¥Ç¥£¥¹¥¯¤Ï PS2 ¤Î¥×¥í¥Æ¥¯¥È¤Î¤»¤¤¤Ç¤Þ¤À¸«¤Æ¤Í¤¨¡£ AV ¥»¥ì¥¯¥¿Çã¤ï¤Ê¤¤¤È¤Ê¤¢¡£
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î25Æü(Æü) [nǯÆüµ­]

#1 [URL] PHP ¥Þ¥Ë¥å¥¢¥ë

¡÷ Namazu ¤Ë¤è¤ë PHP+PostgreSQL ÆüËܸì¥É¥­¥å¥á¥ó¥ÈÁ´Ê¸¸¡º÷¥·¥¹¥Æ¥à:

#2 »ÔµÄ²ñÁªµó

Åêɼ¡£

#3 ¥µ¥Ã¥«¡¼¥Õ¥é¥ó¥¹Àï

ÆâÍƤϤޤÀ¸«¤Æ¤Ê¤¤¤±¤É¡¢5-0 ¤«¡¼¡£ ¤³¤ì¤¬¼ÂÎϺ¹¤Ç¤Ï¤Ê¤¤¤³¤È¤ò¿®¤¸¤¿¤¤¤¬...

#4 [linux] Debian ¤Î ssh ¤Î postinst

¤ä¤Ã¤Èľ¤Ã¤¿¤è¤¦¤À¡£

#5 [dept] ¥µ¡¼¥Ð¥á¥ó¥Æ

ja-man-doc ¤È ja-groff ¤ò package ¤Ç¥¤¥ó¥¹¥È¡¼¥ë¡£ apache ¤ò 1.3.19 ¤Ë¡£

#6 [freshmeat] 3/24 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î26Æü(·î) [nǯÆüµ­]

#1 [linux] migemo

sid ¤Î¥Ñ¥Ã¥±¡¼¥¸¤Ë¤Ê¤Ã¤Æ¤¿¤Î¤ÇÆþ¤ì¤Æ¤ß¤¿¡£ ¤¹¤Ð¤é¤·¤¤¡£ ¹âÎÓ¤µ¤ó±­»ô¤µ¤ó¤¢¤ê¤¬¤È¤ª¡£

#2 [LDP] 3/26 ¤Î updates

#3 [book] Çã¤Ã¤¿ËÜ/Æɤó¤ÀËÜ

Çñ¤Þ¤ê¤¢¤±¤ÎÄ«ÈÓ¿©¤¤¤ËµÈ¾Í»û¤Ë½Ð¤«¤±¤Æ¹ØÆþ¡£Â绶ºâ¡£ ºÇ¶áÆɤó¤À¤Î¤Ç³Ð¤¨¤Æ¤ë¤Î¤Ï ¤¢¤¿¤ê¡£Æ¬»È¤Ã¤Æ¤Ê¤¤¤Ê¡£

º£Æɤó¤Ç¤ë¤Î¤Ï¡Ö¿Í¤Ï¤Ê¤¼¥¨¥»²Ê³Ø¤ËñÙ¤µ¤ì¤ë¤Î¤«¡×¤Î²¼´¬¡£

#4 [linux] sid ¤Î ssh

2.5.2p2-1¡£/etc/ssh/ssh_config ¤Ë
UsePriviledgedPort yes
¤òÄɲ䷤ʤ¤¤È¡¢¸Å¤¤ sshd ¥µ¡¼¥Ð *1 ¤ËÂФ·¤Æ RhostsRSAAuth ¤¬¸ú¤«¤Ê¤«¤Ã¤¿¡£

¡÷ typo:

UsePriviledgedPort ¢ª UsePrivilegedPort ¤Ç¤·¤¿¡£¤´¤á¤ó > masy

*1: potato ¤Î sshd ¥µ¡¼¥Ð´Þ¤à

#5 [freshmeat] 3/25 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#6 ³Ø²Ê¤Î¥¹¥¿¥Ã¥Õ¤¬

¤ªÆó¿ÍÆþ±¡¤µ¤ì¤¿¤ÈÊ̤θ¦µæ¼¼¤Î±¡À¸¤Ëʹ¤¯¡£ ¤À¡¢Âç¾æÉפ«¤·¤é¤ó¡£

#7 [linux] sid ¤Î ptex-bin, jbibtex-bin

tetex-lib ¢ª libkpathsea3, tetex-dev ¢ª libkpathsea-dev ¤¢¤¿¤ê¤ÎÊѹ¹¤Ëȼ¤¤¡¢ °Í¸´Ø·¸¤Î¤»¤¤¤Ç¸½¾õ¥Ð¥¤¥Ê¥ê¤¬ apt ¤Ç¤ÏÆþ¤é¤Ê¤¯¤Ê¤Ã¤Æ¤ë¤¿¤á¡¢ work around ¤È¤·¤Æ¥½¡¼¥¹¤«¤éºî¤Ã¤¿¡£
  1. apt-get source ptex-bin
  2. ptex-bin-2.1.8+1/debian/README.debian ¤òÆɤߡ¢ web2c-src ¤ò¥¤¥ó¥¹¥È¡¼¥ë¡£ tetex-lib, tetex-dev ¤Ï¤â¤¦¤Ê¤¤¤Î¤Ç¡¢ÂåÌò¤Ë libkpathsea3, libkpathsea-dev ¤ò¥¤¥ó¥¹¥È¡¼¥ë (Á°¼Ô¤ÏÉáÄÌÆþ¤Ã¤Æ¤ë¤Ï¤º)¡£
  3. ptex-bin-2.1.8+1/ ¤Ç "dch -v 2.1.8+1-3.0local1" ¤ò¼Â¹Ô¡£ ¥Ð¡¼¥¸¥ç¥ó¤ÏŬµ¹¹¥¤ß¤Î¤â¤Î¤Ë¡£
  4. debuild ¤ò¼Â¹Ô¡£
  5. ¿Æ¥Ç¥£¥ì¥¯¥È¥ê¤Ë jbibtex-bin_2.1.8+1-3.0local1_i386.deb ptex-bin_2.1.8+1-3.0local1_i386.deb ¤¬¤Ç¤­¤ë¤Î¤Ç¡¢ dpkg -i ¤Ç¥¤¥ó¥¹¥È¡¼¥ë
¤È¤¤¤¦´¶¤¸¤Ç¡£

#8 [thesis] pdf ²½

ps2pdf ¤Ç´Êñ¤Ë¤Ç¤­¤ë¤Î¤À¤Ê¤¢¡£ Îã¤Î̵°ÕÌ£¤Ë¤Ç¤«¤¤ PS ¤Î¤»¤¤¤Ç¡¢ dvi2ps ¤Ê¥Õ¥¡¥¤¥ë¤Ï 48M ¤â¤¢¤ë¤Î¤À¤¬¡¢ pdf ¤Ë¤·¤¿¤é 2.8M Äø¤Ë¤Ê¤Ã¤¿¡£ ¤â¤Á¤í¤ó¸«¤¿ÌܤϤÁ¤ç¤Ã¤ÈÍî¤Á¤ë¤¬¡¢ pdf ¤Î¤Û¤¦¤¬°õºþ¤â®¤¤¤è¤¦¤Êµ¤¤¬¤¹¤ë¡£
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î27Æü(²Ð) [nǯÆüµ­]

#1 [LDP] 3/27 ¤Î updates

#2 [URL] ¥¤¥ó¥¿¡¼¥Í¥Ã¥È¤Ç¸ë¤òÂǤȤ¦!

sid ¤Î cgoban ¤È¤«¤Ç¤Ä¤Ê¤²¤ë¤Î¤«¤Ê¡© gnugo-dv ¤ÈÂжɤ·¤Æ¤ß¤¿¤é¡¢ 9 Ï©È×ÄêÀè¤ÎÇò¤Ç 5 ²ó¤ä¤Ã¤Æ 1 ²óÉԳФò¼è¤Ã¤¿¡£

#3 [thesis] °õºþ¤·¤¿¤é

¤ä¤ëµ¤¤¬½Ð¤Æ¤­¤¿(¤ï¤é
¤Á¤ç¤Ã¤ÈÊä´°¤·¤¿¤¤¥Ç¡¼¥¿¤òºî¤ë batch job ¤ò quick hack ¤·¤ÆÆͤùþ¤à¡£ ¤°¤¦Ì²¤¤¡£

#4 [freshmeat] 3/26 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î28Æü(¿å) [nǯÆüµ­]

#1 [LDP] 3/28 ¤Î updates

#2 [paper] RSI 72(4) April 2001

¡÷ An apparatus for the measurement of internal stress and thermal expansion coefficient of metal oxide films:

Cheng-Chung Lee, Chuen-Lin Tien, Wean-Shyang Sheu and Cheng-Chung Jaing; pp.2218-2133
A measuring apparatus based on a phase shifting interferometry technique to determine the mechanical properties of metal oxide films was presented. Thin films were prepared by ion-beam sputter deposition at low substrate temperature. Quantitative determination of the mechanical properties such as the internal stress, biaxial elastic modulus, and thermal expansion coefficient of metal oxide films were investigated. A phase shifting Twyman˨reen interferometer with the phase reduction algorithm was setup to measure the temperature-dependent stress in thin films. Two types of circular glass plates, with known Young's moduli, Poisson's ratios, and thermal expansion coefficients, were used as coating substrate. The temperature-dependent stress behavior of the metal oxide films was obtained by heating samples in the range from room temperature to 70 ¡ÝC. The stresses of thin films deposited on two different substrates were plotted against the stress measurement temperature, showing a linear dependence. Four oxide films were reported for their film stresses and thermal expansion coefficients.

¡÷ Data reduction in 3¦Ø method for thin-film thermal conductivity determination:

T. Borca-Tasciuc, A. R. Kumar, and G. Chen pp. 2139-2147
The 3¦Ø method has been proven to be very useful for determining the thermal conductivity of thin films and their substrates. Several simplifications are often used in determining the thermal conductivity of the films based on the experimentally measured 3¦Ø signal. These simplifications, however, have limited range of applicability. In this work, we present a detailed analysis and mathematical modeling of the 3¦Ø method applied for different experimental conditions. Effects considered include the finite substrate thickness, anisotropic nature of the film and substrate thermal conductivity, the film-substrate thermal property contrasts, the effect of heat capacitance of the heater, and the effect of thermal boundary resistance. Several experimental results are analyzed using the models presented. This work shows that the 3¦Ø method can be extended to a wide range of sample conditions, with anisotropic conductivities in both the substrate and the film, and with small film-substrate conductivity contrast.

#3 [labo] ¥á¥â¥êÁýÀß

Ä«¤Ã¤Ñ¤é(¾Ð)¤«¤é¡¢ Àè·î Çã¤Ã¤¿ 128M ¥á¥â¥ê¤ò¿È¤Î¼þ¤ê¤Î¥Þ¥·¥ó¤ËÁýÀß¡£ °ìÈÖ²÷Ŭ¤Ë¤Ê¤Ã¤¿¤Î¤Ï windows ¤À¤Ã¤¿¤ê¡£ ¥Õ¥¡¥¤¥ë¥µ¡¼¥Ð¤â¤³¤ì¤Ç¥­¥ã¥Ã¥·¥å¤¬¸ú¤¤¤Æ·Ú¤¯¤Ê¤Ã¤Æ¤¯¤ì¤ë¤È¤¤¤¤¤Ê¡£

#4 [labo] ²Ê¸¦Èñ¼ý»ÙÊí

¤Þ¤È¤á¤¿¡£¤¢¤È¤Ï¥Õ¥ë¥¦¥Á¤ÎÎμý½ñÂÔ¤Á¡£

#5 Êݸ±°ú¤­Íî¤È¤·

µëÎÁ¤Î¿¶¹þ¸ýºÂ¤òÊѤ¨¤¿¤Î¤Ç¡¢¶â¤¬Â­¤ê¤º¤ËÍî¤Á¤Ê¤«¤Ã¤¿¤é¤·¤¤(^^; ¸½¶â¤ÇÂåÍýŹ¤Ë»ý¤Ã¤Æ¤¤¤¯¤³¤È¤Ë¡£

#6 [freshmeat] 3/27 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

¡÷ nslint:

»î¤·¤Æ¤ß¤¿¡£¥¨¥é¡¼¤¬¤Ò¤È¤Ä¸«¤Ä¤«¤Ã¤¿(^^; debian ¤À¤È named.conf ¤Î°ÌÃÖ¤¬ ISC ¤Î¥Ä¥ë¥·¤Î¤È¤Ï°ã¤¦¤Î¤Ç¡¢
nslint -b /etc/bind/named.conf
¤Î¤è¤¦¤Ëµ¯Æ°¤¹¤ëɬÍפ¬¤¢¤ë¡£ ¤·¤«¤· documentation ¤¬°µÅÝŪ¤Ë¾¯¤Ê¤¤¤Ê¡£ ¤¤¤¤¥×¥í¥°¥é¥à¤Ê¤Î¤À¤¬¡¢¤â¤Ã¤¿¤¤¤Ê¤¤¡£

¤¤¤ä¡¢man ¤¬¤¢¤ë¤Î¤«¡£¤Õ¤à¤Õ¤à¡£

¤È¤¤¤¦¤« deb ¤â¤¢¤Ã¤¿¤Î¤«(^^;

#7 [thesis] bem vs diff ¤Î³¨

¤¬¡¢¤Ç¤­¤¿¡£¤¦¤à¤¦¤à¡£
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î29Æü(ÌÚ) [nǯÆüµ­]

#1 [LDP] 3/29 ¤Î updates

#2 [labo] APS March Meeting - MgB2 Post deadline session

¹Ö±é¤¬ RealAudio ¤Ç¼ýÏ¿¤µ¤ì¤Æ¤¤¤ë¡£¤¹¤´¤¤¤Ê¡£

#3 [linux] mh has been orphaned

¤Þ¤¢Ã¯¤«¤¬ take over ¤·¤Æ¤¯¤ì¤ë¤¸¤ã¤í¡¢¤È³Ú´Ñ(^^;

#4 [linux] sid's xlib 4.0.2-12 conflicts with jgroff?

% sudo apt-get upgrade
Reading Package Lists... Done
Building Dependency Tree... Done
1 packages upgraded, 0 newly installed, 0 to remove and 2  not upgraded.
Need to get 0B/1170kB of archives. After unpacking 0B will be used.
Do you want to continue? [Y/n]
(¥Ç¡¼¥¿¥Ù¡¼¥¹¤òÆɤ߹þ¤ó¤Ç¤¤¤Þ¤¹... ¸½ºß 62021 ¸Ä¤Î¥Õ¥¡¥¤¥ë¤È¥Ç¥£¥ì¥¯¥È¥ê¤¬¥¤¥ó¥¹
¥È¡¼¥ë¤µ¤ì¤Æ¤¤¤Þ¤¹¡£)
xlibs 4.0.2-11 ¤ò(.../xlibs_4.0.2-12_i386.deb ¤Ç)ÃÖ´¹¤¹¤ë¤¿¤á¤Î½àÈ÷¤ò¤·¤Æ¤¤¤Þ¤¹.
..
xlibs ¤òŸ³«¤·¡¢ÃÖ´¹¤·¤Æ¤¤¤Þ¤¹...
dpkg: /var/cache/apt/archives/xlibs_4.0.2-12_i386.deb ¤ÎÆɤ߹þ¤ß¥¨¥é¡¼¤Ç¤¹(--unp
ack) `/usr/X11R6/lib/X11/app-defaults'¤ò¾å½ñ¤­¤·¤è¤¦¤È¤·¤Æ¤¤¤Þ¤¹¡£¤³¤ì¤Ï¥Ñ¥Ã¥±¡¼
¥¸ jgroff ¤Ë¤â´Þ¤Þ¤ì¤Æ¤¤¤Þ¤¹¡£¡£
°Ê²¼¤Î¥Ñ¥Ã¥±¡¼¥¸¤Î½èÍýÃæ¤Ë¥¨¥é¡¼¤¬È¯À¸¤·¤Þ¤·¤¿:
 /var/cache/apt/archives/xlibs_4.0.2-12_i386.deb
E: Sub-process /usr/bin/dpkg returned an error code (1)

¡÷ °ã¤Ã¤¿:

sid ¤Ç¤Ï¤â¤¦ jgroff ¤Ï groff ¤Ë¤Ê¤Ã¤Æ¤¿¡£ potato ¤«¤é dist-upgrade ¤·¤¿¤È¤­¤Ë¤Ê¤ó¤«»Ä³¼¤¬»Ä¤Ã¤Æ¤¿¤é¤·¤¤¡£
dpkg --purge --force-depends jgroff
apt-get install jgroff
¤Ç jgroff ¤ÎÂå¤ï¤ê¤Ë groff ¤¬Æþ¤Ã¤Æ°ì·ïÍîÃå¡£

¡÷ ¤¤¤ä:

apt-get install groff
¤À¤±¤Ç¤ª¤Ã¤±¡¼¤À¤Ã¤¿¡£

#5 [linux] Samba ¤Î LDAP ǧ¾Ú

PAM ¤ÈÁȤ߹ç¤ï¤»¤ë¤È¤Ç¤­¤ë¤ó¤Ç¤Ê¤¤¤«¤Ê¡¢¤È¤¤¤¦µ¤¤Ï¤·¤Þ¤¹¤Ç¤¹¤Í¡£ ¤³¤Î¤Ø¤ó ¤È¤« ¤³¤Î¤Ø¤ó ¤È¤«¤«¤Ê¡©

¤·¤«¤· pam ¤â ldap ¤â¤è¤¯¤ï¤«¤Ã¤È¤é¤ó¤Î¤Ç¥¢¥ì¡£

¡÷ ¤È¤¤¤¦¤³¤È¤Ç:

apt-get install libpam-doc ¤·¤Æ¤ß¤¿¤ê¡£ ldap ¤Ï¤É¤Ã¤«¤Ë LC 2000 fall ¤Ç¤Î±­»ô¤µ¤ó¤Î¹Ö±éµ­Ï¿¤¬¤¢¤Ã¤¿µ­²±¤¬... Í­ÎÁ¤À¤Ã¤¿¤«¤é¤À¤á¤«¤Ê¡©

#6 [paper] JAP 89(7) 1 April 2001

¡÷ Electric field in inductively coupled gas discharges:

R. Piejak, V. Godyak, and B. Alexandrovich; pp.3590-3593
The electric field in a low-pressure electrodeless discharge has been determined from discharge voltage measurements at constant discharge current as a function of gas pressure. Measurements have been made in neon, argon, and xenon at discharge currents of 1, 3, and 10 A with a driving frequency of 0.45 MHz. The behavior of the electric field as a function of gas pressure has been found to be qualitatively similar for all three gases. At the lowest gas pressures at which a discharge can be sustained, the electric field is relatively high. With increasing gas pressure the field reaches a local minimum, followed by a local maximum and another local minimum. Above 1 Torr, the electric field increases monotonically with gas pressure.

¡÷ Practical scheme for three-dimensional simulation of electron cyclotron resonance plasma reactors:

Yasuyoshi Yasaka and Nobuki Uda; pp.3594-3601
A three-dimensional simulation code which calculates wave propagation, plasma transport, and gas phase chemical reactions self-consistently in an electron cyclotron resonance plasma reactor has been developed. The code is designed to treat the three-dimensional inhomogeneity with a reasonable accuracy in a realistic configuration of the reactor within an acceptable computational time using common computer resources. The profiles of electromagnetic wave fields and the temporal evolution of plasma parameters and radical densities in a bounded, inhomogeneous, cylindrical system have been calculated. The code can resolve azimuthal asymmetry of the plasma associated with a rectangular waveguide coupling or an asymmetric injection of reactive gases as well as the radial and axial variations.

¡÷ Superhardness effects of heterostructure NbN/TaN nanostructured multilayers:

Junhua Xu, Masao Kamiko, Yaomin Zhou, Ryoichi Yamamoto, Geyang Li and Mingyuan Gu; pp. 3674-3678
Although superhardness effects have been extensively investigated for epitaxial ceramic nanomultilayer films with the same crystal structures in the last decade, those for multilayers with different crystal structures have been seldom studied. In this article, NbN/TaN nanomultilayers have been designed and deposited by reactive magnetron sputtering. The results showed that the crystal structures of NbN and TaN are face-centered cubic and hexagonal in superlattice films, respectively, and the lattice plane (111) of NbN is coherent with the (110) of TaN, i.e., {111}fcc-NbN{110}h-TaN. The results of microhardness measurement showed that the superhardness effects of NbN/TaN multilayers exist in a wide range of modulation period from 2.3 to 17.0 nm. This phenomenon is different from that of epitaxial ceramic multilayers where the maximum hardness usually takes place at a modulation period of 5.0?10.0 nm. It is proposed that the coherent stresses and the structural barriers (fcc/hexagonal) to dislocation motion between NbN and TaN layers are the main reasons for the high-hardness value in a wide range of modulation periods.

¡÷ Design and characterization of thin film microcoolers:

Chris LaBounty, Ali Shakouri and John E. Bowers; pp. 4059-4064
Thin film coolers can provide large cooling power densities compared to bulk thermoelectrics due to the close spacing of hot and cold junctions. Important parameters in the design of such coolers are investigated theoretically and experimentally. A three-dimensional (3D) finite element simulator (ANSYS) is used to model self-consistently thermal and electrical properties of a complete device structure. The dominant three-dimensional thermal and electrical spreading resistances acquired from the 3D simulation are also used in a one-dimensional model (MATLAB) to obtain faster, less rigorous results. Heat conduction, Joule heating, thermoelectric and thermionic cooling are included in these models as well as nonideal effects such as contact resistance, finite thermal resistance of the substrate and the heat sink, and heat generation in the wire bonds. Simulations exhibit good agreement with experimental results from InGaAsP-based thin film thermionic emission coolers which have demonstrated maximum cooling of 1.15 ¡î at room temperature. With the nonideal effects minimized, simulations predict that single stage thin film coolers can provide up to 20-30 ¡î degrees centigrade cooling with cooling power densities of several 1000 W/cm^2.

¡÷ Secondary electron emission yields from MgO deposited on carbon nanotubes:

Whikun Yi, et al.; pp. 4091-4095
Enormously high secondary electron emission yields under electric field are observed from MgO deposited on carbon nanotubes. The yields reach a value as high as 15 000 and are strongly dependent upon the bias voltage applied to the sample. The creation of the electric field across the MgO film after bombardment of primary electrons is considered as one of key features, since positive charges are generated at the surface by departure of secondary electrons. Subsequent bombarding electrons produce other secondary electrons inside the MgO film, then the liberated secondaries are accelerated towards the surface under the strong field. Under this condition, the secondary electrons gain sufficient energy to create further electrons by impact ionization. The process continues until an equilibrium avalanche is established. To elucidate the earlier explanations, the kinetic energy spectra of secondary electrons are measured by an energy analyzer at various bias voltages in MgO/carbon nanotube samples. The analysis of spectral results with the energy band diagram gives us strong evidence for the suggested mechanism.

¡÷ Formation of ¦Â-C3N4 crystals at low temperature:

J. Wei; pp. 4099-4104
Carbon nitride films with ¦Â-C3N4 crystals of 200 nm grain size were grown on Si (100) substrates using magnetron sputtering. Reactive deposition was achieved using a graphite target in an argon/nitrogen plasma at room temperature. These films were characterized by transmission electron microscopy (TEM), atomic force microscopy (AFM), x-ray photoelectron spectroscopy (XPS), Fourier-transform infrared spectroscopy (FTIR), and Raman spectroscopy. Micro level ¦Â-C3N4 crystal grains were observed with TEM. According to calculations from electron diffraction pattern, these crystalline structures were in a good agreement with hypothetical b-C3N4 structure. AFM measurement also indicated the grain size was around 200 nm and the carbon nitride films had low surface roughness. From XPS data, maximum N/C ratio of 0.5 was achieved in the films. XPS spectra of the films typically showed three peaks in the C 1s core level spectrum (centered at 284.6, 285.9, and 287.2 eV) and two peaks in the N 1s core level spectrum (centered at 398.7 and 400.2 eV). This indicates that there are two types of C-N bonds; N is bonded to sp2- or sp3-coordinated C atoms in the as-deposited films. FTIR spectra showed three absorption bands in the range of 1000?3000 cm?1. The absorption band around 2367 cm?1 can be attributed to CN nitrile bond. The absorption bands around 1559 and 1201 cm?1 demonstrate the existence of CN (sp2) and C?N (sp3) bonds. Analysis of Raman spectrum further demonstrated the coexistence of sp, sp2, and sp3 bonds. All of XPS, FTIR, and Raman measurements showed the presence of fourfold coordinated ¦Â-C3N4 crystals in the films, which is in good agreement with TEM and electron diffraction results.

¡÷ Sputtering and in-plane texture control during the deposition of MgO:

Liang Dong, Luis A. Zepeda-Ruiz and David J. Srolovitz; pp. 4105-4112
iMolecular dynamics simulations are performed to study the fundamental role of the ion beam in determining the in-plane texture of 100 oriented (out-of-plane) MgO films during ion beam assisted deposition (IBAD). Sputter yields are determined as a function of in-plane orientation for Ar ion beams. The minimum sputter yield exists at an ion beam orientation corresponding to the MgO 110 direction. The finite width of the sputter yield minimum is attributable to two main factors: (i) only a fraction of the incident ions are oriented to travel directly down the center of the channel and (ii) ions that are not exactly parallel to the channeling direction may channel. While the simulations imply that it is possible to in-plane orient {001} MgO films using IBAD, there are fundamental limitations on the degree of ordering that can be achieved.

#7 [labo] ²Ê¸¦Èñ¼ý»ÙÊí

Äó½Ð¡£ ¥Õ¥ë¥¦¥Á¤ÎÎμý½ñ¤Ï boss ¤Î¥Ý¥¹¥È¤Ë´Ö°ã¤Ã¤ÆÆþ¤Ã¤Æ¤¤¤¿¡£¤¦¤Ì¤Ì¡£

¡÷ Äó½ÐÀè¤Ç:

³ØÉôŤËÊá¤Þ¤Ã¤Æ(¤ï¤é¡¢¥³¡¼¥Ò¡¼¤ò¤´ÃÚÁö¤Ë¤Ê¤Ã¤¿¡£
¤¤¤í¤¤¤í¤Ê¤È¤³¤í¤¬¤¤¤í¤¤¤íÂçÊѤ餷¤¤¤Ê¤¢(Ææ

#8 [freshmeat] 3/28 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#9 [linux] sarg

sid ¤Î¥Ñ¥Ã¥±¡¼¥¸¤Ë¤Ê¤Ã¤Æ¤¿¤Î¤Ç¡¢ potato ¤Ç¥³¥ó¥Ñ¥¤¥ë¤·¤Æ¥¤¥ó¥¹¥È¡¼¥ë¤·¤Æ¤ß¤¿¡£ ¼Â¤ËÎɤ¤´¶¤¸¡£ squid ¤Î log analysis tool ¤Ï¿ô¼ïÎà»î¤·¤Æ¤ß¤¿¤³¤È¤¬¤¢¤ë¤¬¡¢¤½¤ÎÃæ¤Ç best¡£

¡÷ peer host ¤«¤é¤Î query ¤Î exclude:

¥Ç¥Õ¥©¥ë¥È¤À¤È ICP_QUERY ¤ò¤è¤³¤¹ sibling ¤Ê squid ¥Û¥¹¥È¤«¤é¤ÎÌä¹ç¤ï¤»¤â¥í¥°¤Ë¥«¥¦¥ó¥È¤µ¤ì¤Æ¤·¤Þ¤¦¤¬¡¢ /etc/squid/sarg.users *1 ¤Ë¤½¤Î¥Û¥¹¥È̾ (¤È IP ¥¢¥É¥ì¥¹) ¤ò½ñ¤¯¤È OK ¤È¤Ê¤Ã¤¿¡£

¤Á¤Ê¤ß¤Ë¤³¤ì¤é¤Î¥Õ¥¡¥¤¥ë¤Ë¶õ¹Ô¤òÆþ¤ì¤Æ¤·¤Þ¤¦¤È¡¢ ¤¢¤é¤æ¤ë¹Ô¤Ë¥Þ¥Ã¥Á¤·¤Æ¥í¥°½ÐÎϤ¬°ìÀڽФʤ¯¤Ê¤Ã¤Æ¤·¤Þ¤¦¡£

*1: ¤Ê¤¼ sarg.hosts ¤Ç¤Ï¤Ê¤¤¤Î¤À¤í¤¦...
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î30Æü(¶â) [nǯÆüµ­]

#1 [paper] cond-mat

¡÷ 0103475: Coulomb Explosion and Thermal Spikes:

A fast ion penetrating a solid creates a track of excitations. This can produce displacements seen as an etched track, a process initially used to detect energetic particles but now used to alter materials. From the seminal papers by Fleischer et al. [Phys. Rev. 156, 353 (1967)] to the present [C. Trautmann, S. Klaumunzer and H. Trinkaus, Phys. Rev. Lett. 85, 3648 (2000)], `Coulomb explosion' and thermal spike models are treated as conflicting models for describing ion track effects. Here molecular dynamics simulations of electronic-sputtering, a surface manifestation of ion track formation, show that `Coulomb explosion' produces a `heat' spike so that these are early and late aspects of the same process. Therefore, differences in scaling are due to the use of incomplete spike models.

#2 [JF] NIS-HOWTO

¥ê¥ê¡¼¥¹¡£¾®ÎÓ¤µ¤ó¤Î¤ª¤«¤²¡£

#3 [book] ¡Ø¿Í¤Ï¤Ê¤¼¥¨¥»²Ê³Ø¤ËñÙ¤µ¤ì¤ë¤Î¤«¡Ù¥«¡¼¥ë¡¦¥»¡¼¥¬¥óÃø ÀÄÌÚ·° Ìõ ¿·Ä¬Ê¸¸Ë

Éð°æ¤µ¤ó¤ÎÆüµ­ ¤Çʸ¸Ë²½¤òÃΤꡢ¹ØÆþ¡¢ÆÉλ¡£ ¤³¤ÎËܤǸÀ¤Ã¤Æ¤ëÆâÍƤäƤΤϡ¢ ¤«¤Ê¤ê¼«Ê¬¤Î»ý¤Ã¤Æ¤ë¿®¾ò¤Ë¶á¤¤¤Î¤Ç¡¢ Æɤó¤Ç¤¤¤Æ¡ÖÌؤò·¼¤«¤ì¤¿¡×¤È¤¤¤¦´¶¤¸¤Ç¤Ï¤Ê¤«¤Ã¤¿¡£ ¤¿¤À¡¢¥¢¥¤¥Ç¥¢¤¬ÌÀ³Î¤Ëʸ¾Ï²½¤µ¤ì¤Æ¤¤¤ë¡¢ ¤È¤¤¤¦ÅÀ¤Ç¤Î²ÁÃͤÏÈó¾ï¤ËÂ礭¤¤¤È»×¤¦¤·¡¢ ¾­Í輫ʬ¤¬°úÍѤ·¤ÆÍøÍѤǤ­¤ë¤È¤¤¤¦°ÕÌ£¤Ç¤â ¤¢¤ê¤¬¤¿¤¤Ëܤˤʤꤽ¤¦¤À¡£

²Ê³Ø¤¬°Í¤Ã¤ÆΩ¤Ä¤È¤³¤í¤Î²ûµ¿¼çµÁ¤Ê¤¯¤·¤Æ¤Ï¡¢ Âç½°¤Î°Õ¼±¤¬»ÙÇÛÁؤˤè¤ê¥³¥ó¥È¥í¡¼¥ë¤µ¤ì¤ë¼Ò²ñ¤¬ÅþÍ褷¤Æ¤·¤Þ¤¦¡¢ ¤È¤¤¤¦¤Î¤¬¸åȾ¤Ç¿¤¯¤ÎÊǤò³ä¤¤¤Æ½Ò¤Ù¤é¤ì¤Æ¤¤¤ë¤È¤³¤í¡£ ¤³¤Î¥»¡¼¥¬¥ó¤Î´íµ¡°Õ¼±¤Ï¡¢ Âç³ØÀ¸ (¤¢¤ë¤¤¤ÏÂç³Ø±¡À¸¤Ç¤¹¤é) ¤òÁê¼ê¤Ë¤·¤Æ¤Æ¤µ¤¨¡¢ ¤Ò¤·¤Ò¤·¤È´¶¤¸¤ë¡£ *1 ¼ã¤¤ÁؤËÂФ·¤Æ¶¯¤¯¤¹¤¹¤á¤¿¤¤¡£

¤Ê¤ª¡¢ËÝÌõ¤Î¼Á¤âÈó¾ï¤Ë¹â¤¤¡£ ¤Ç¤âÌõ¼Ô¤¢¤È¤¬¤­¤Ë¤¢¤ë
¥Ð¥¹¥±¥Ã¥È¥Ü¡¼¥ë¤ÎÏäòÌõ¤¹¤¿¤á¤Ë¡¢
(Ãæά)
¡Ø¥¹¥é¥à¡¦¥À¥ó¥¯¡ÙÁ´»°½½°ì´¬¤òÆÉÇˤ·¤Æ¤·¤Þ¤Ã¤¿¡£
¤Ã¤Æ¤Î¤Ï¤ä¤ê¤¹¤®¤À¤È»×¤¦¡£ ¤Æ¤¤¤¦¤«¤½¤ì¤ÏËÝÌõ¤È¤Ï´Ø·¸¤Ê¤¤¤À¤í(¾Ð)
*1: ¡Ö¿·Ê¹¤Ë½ñ¤¤¤Æ¤¢¤ë¤³¤È¤Ã¤ÆÁ´ÉôÀµ¤·¤¤¤ó¤Ç¤¹¤è¤Í¡× ¤È¤«¤¤¤¦Âç³Ø±¡À¸¤¬ËÜÅö¤Ë¤¤¤ë¤Î¤À¡£

#4 [labo] Agilent IntuiLink

¥¢¥¸¥ì¥ó¥È¡¦¥Æ¥¯¥Î¥í¥¸¡¼³ô¼°²ñ¼Ò¤Ï¡¢ ¥¢¥¸¥ì¥ó¥È¡¦¥Æ¥¯¥Î¥í¥¸¡¼À½¤Î¬Äê´ï¤È PC¥¢¥×¥ê¥±¡¼¥·¥ç¥ó¤È¤Î¥Ç¡¼¥¿¤Î¼õ¤±ÅϤ·¤òÍưפˤ¹¤ë¥½¥Õ¥È¥¦¥§¥¢ ¡ÖAgilent IntuiLink¡Ê¥¤¥ó¥Á¥å¥¤¥ê¥ó¥¯¡Ë¡×¤òȯɽ¡¢Ìµ½þÄ󶡤ò³«»Ï¤·¤Þ¤·¤¿¡£
ÂбþºÑ¤ßÀ½Éʥꥹ¥È:

#5 [freshmeat] 3/29 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#6 [linux] bind ¤Î chroot ²½

debian-users ¤Ç ÃÑ ¤ò »¯ ¤·¤Æ ¤·¤Þ¤Ã¤¿¤Î¤Ç¡¢ ²ù¤·Ê¶¤ì¤Ë¼ê¸µ¤Ç¼Â¹Ô¡£

¾ðÊó¸»¤Ï Chroot-BIND-HOWTO ¤È¤« Linux.com ¤Îµ­»ö ¤È¤«¡£

¡÷ user/group named ¤ÎÄɲÃ:

/etc/passwd:
named:*:35:35:Nameserver:/chroot/bind:/bin/sh
/etc/group:
named:*:35:

¡÷ ¥Ç¥£¥ì¥¯¥È¥ê¤Î½àÈ÷:

¤¦¤Á¤Ï / ¤È /usr ¤¬Ê̥ѡ¼¥Æ¥£¥·¥ç¥ó¤Ê¤Î¤Ç¡¢ln ¤È cp ¤Ï¤½¤Î¤Ø¤ó (¤È¥Õ¥¡¥¤¥ë¤ÎÂ礭¤µ) ¤òÈ¿±Ç¤·¤Æ¤¤¤ë¡£ (3/31: ln ¤·¤Æ¤Ï¤À¤á¡£ cp ¤Ë½¤Àµ¡£)
# mkdir -p /chroot/bind; cd /chroot/bind
# mkdir -p sbin usr/sbin etc dev lib

# cp /sbin/ldconfig sbin

# cp /usr/sbin/named usr/sbin
# cp /usr/sbin/named-xfer usr/sbin

# cp -r /etc/bind etc
# chown -R named.named etc/bind
# cp /etc/localtime etc

# mkdir var/cache/named var/run
# chown named.named var/cache/named var/run

# cd lib
# cp /lib/libc-2.1.3.so .
# ln -s libc-2.1.3.so libc.so.6
# cp /lib/ld-2.1.3.so .
# ln -s ld-2.1.3.so ld-linux.so.2

# cd ../dev
# mknod null c 1 3
# chmod 666 null
ls -lR /chroot/bind | grep -v "^total" ¤Î·ë²Ì¤Ï ¤³¤Á¤é ¡£¤¿¤À¤·¸å½Ò¤Î dev/log ¤È¤«¡¢ ¼Â¹Ô»þ¤Ë¤Ç¤­¤ë var/run °Ê²¼¤Î¥Õ¥¡¥¤¥ë¤âÆþ¤Ã¤Æ¤¤¤ë¡£

¡÷ ld.so.cache ¤ÎºîÀ®:

# chroot /chroot/bind /sbin/ldconfig -v
¤È¤·¤Æ¡¢/chroot/bind/etc/ld.so.cache ¤òºî¤ë¡£

¡÷ syslog ¤Ø¤Î¥Ç¥Ð¥¤¥¹ÄɲÃ:

/etc/init.d/sysklogd ¤Î SYSLOGD ¤ÎÄêµÁ¤ò
SYSLOGD="-a /chroot/bind/dev/log"
¤È¤·¤Æ /etc/init.d/sysklogd restart¡£ ¤¹¤ë¤È /chroot/bind/dev/log ¤¬¤Ç¤­¤ë¤Ï¤º¡£

¡÷ /etc/init.d/bind ¤Î½ñ¤­ÊѤ¨:

·ë²Ì¤À¤±¼¨¤¹¤È ¤³¤Á¤é ¡£ndc ¤Î -c, -n, -p ³Æ¥ª¥×¥·¥ç¥ó¤¬¥ß¥½¡£ -n ¥ª¥×¥·¥ç¥ó¤Ã¤Æ undocumented ¤Ê¤Î¤À¤¬¡£

¤¢¤È¤Ï /etc/init.d/bind {start|reload|restart} ¤Ê¤É¤¬ÉáÄ̤˻Ȥ¨¤ë¡£ µ¯Æ°»þ¤Î /var/log/daemon.log ¤Î¥¨¥ó¥È¥ê¤Ï ¤³¤ó¤Ê ¤«¤ó¤¸¡£chroot ¤·¤Æ¤¤¤ë¤³¤È¤¬¤ï¤«¤ë¤È»×¤¦¡£

/usr/sbin ¤Î bind ¤È bind-xfer ¤Ï chmod -x ¤·¤Æ¤ª¤¯¤È¤¤¤¤¤«¤â¡£

#7 [thesis] ËÜÆü¤ÎÀ®²Ì

¤Õ¡¼¡¢»Ä¤ë¤Ï¤¢¤È»°Ëç¡£
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

2001ǯ03·î31Æü(ÅÚ) [nǯÆüµ­]

#1 Ä«

µ¯¤­¤¿¤éÀ㤬¹ß¤Ã¤Æ¤¤¤Æ¤Ó¤Ó¤ë¡£

¡÷ Ãë:

ºù¤Î³«²ÖÆü¤Î¸å¤ËÀ㤬¹ß¤Ã¤¿¤Î¤Ï 25 ǯ¤Ö¤ê¤é¤·¤¤¡¢ ¤ÈÅìµþ³¤¾å¤Î¤ª¤¸¤µ¤ó¤«¤éʹ¤¤¤¿¡£

#2 [linux] bind ¤Î chroot ²½¤Ë¤ª¤±¤ë ln ¤È cp

¤Ð¤«¤À¤Ê > ²¶
¤»¤Ã¤«¤¯ chroot jail ¤ÎÃæ¤ËÆþ¤ì¤Æ¤ë¤Î¤Ë¡¢ libc ¤Ê¤ó¤Æ critical ¤Ê¥Ö¥Ä¤ò³°Éô¤È common ¤Ë¤·¤Æ¤¤¤ë¤ó¤¸¤ã ²ÁÃÍȾ¸º¤¸¤ã¤ó¡£ ¤Ä¡¼¤³¤È¤Çµ­½Ò¤Ï½¤Àµ¤·¤Æ¤ª¤¤¤¿¡£

#3 ¥â¥¹¥Ð¡¼¥¬¡¼À®ìþÂç³ØÁ°Å¹

º£Æü¤ÇÊÄŹ¤À¤½¤¦¤À¡£¤Þ¤¿µ®½Å¤ÊÈӤξì½ê¤¬...

#4 [book] ¥Ñ¥í¥Ç¥£ÈÇ BSD magazine

¥Ñ¥ë¥³¥Ö¥Ã¥¯¥»¥ó¥¿¡¼¤ÇÆþ¼ê¡£

ÃëÈÓ¤ò¿©¤¤¤Ê¤¬¤éÆɤó¤Ç¤¤¤¿¤Î¤Ç¡¢ °ìÈÖÌÌÇò¤«¤Ã¤¿¤Î¤Ï "Debugging The Food"¡£Ã¯¤À¤í¤³¤ì½ñ¤¤¤¿¤Î :-) °ìÈ֤Ĥޤé¤Ê¤«¤Ã¤¿¤Î¤Ï IP ¥Þ¥Í¡¼¡£

Æî¿·½É¥¢¥É¥Ù¥ó¥Á¥ã¡¼¤Ï sid ¤Ç¥Ó¥ë¥É¤Ç¤­¤¿¡£ uudeview ¤Ç decode ¤·¡¢ libreadline4, libreadline4-dev ¤ò apt-get install¡¢ make ¤Ç OK¡£

#5 [JF] resolve some reservations

2.2.19 ¤Î Changes ¤ò¥ê¥ê¡¼¥¹¡¢ TT-Debian ¤Ï obsolete/ ¹Ô¤­¤Ë¤·¤¿¡£ ¤³¤ì¤Ç JF ¤Î´Ø·¸¤Î̤·è°Æ·ï¤Ï̵¤·¡£

#6 [freshmeat] 3/30 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#7 [linux] dvorak7min

debian ¤Î¥Ñ¥Ã¥±¡¼¥¸¤Ë¤Ê¤Ã¤Æ¤¿¤Î¤Ç»î¤·¤Æ¤ß¤¿¤¬¡¢ man ¤·¤Æ¤ß¤¿¤È¤³¤í
dvorak7min assumes it is run with the dvoarak keymappings already loaded.
¤È¤¤¤¦¤³¤È¤Ç¡¢µ¯Æ°¤Ç¤­¤Í¤¨(¾Ð)

#8 [JM] LDP man-pages 1.35

¤é¤·¤¤¡£¤¦¤à¤à¡£

¤Ö¤Ï LDP.7 ¤È¤«Æþ¤Ã¤Æ¤ë(¾Ð)

¤È¤ê¤¢¤¨¤º basename.3 ¤Ë¤¶¤Ã¤ÈÌõ¤òÉÕ¤±¤ÆÅꤲ¡£

lilo ´Ø·¸¤Î¥Þ¥Ë¥å¥¢¥ë¤¬ LDP ¤Î archive ¤«¤é¤Ï¤Ê¤¯¤Ê¤Ã¤¿¤é¤·¤¤¤Î¤Ç¡¢ ¿·¤¿¤Ë lilo-21.7 ¤«¤é import ºî¶È¡£·ë¹½ÊѤï¤Ã¤Æ¤ë¤Ê¡£

#9 [paper] PHYSICAL REVIEW FOCUS 30 MAR 2001

¡÷ INTERNET PLAGUES SPREAD RAPIDLY:

If there's an outbreak of the flu in your city, you can count on the Centers for Disease Control for help, but if it's the "I Love You" bug, forget it. That's because viruses spread differently on the internet than they do in the real world, according to a paper in the 2 April PRL. While a biological disease can only spread from person to person, a digital virus can reach many computers simultaneously from a single server. This difference in transmission makes computer viruses all but impossible to eliminate, according to the authors, but the model they describe may lead to better strategies for protecting the electronic world.
(R. Pastor-Satorras and A. Vespignani, Phys. Rev. Lett. 86, 3200. )

¤Õ¤Õ¤Õ¡£
¥³¥á¥ó¥È [Á´ÉôÆɤà/Åê¹Æ¤¹¤ë]

°Ê¾å¡¢11 Æüʬ¤Ç¤¹¡£
¥¿¥¤¥È¥ë°ìÍ÷
¥«¥Æ¥´¥êʬÎà
book
dept
issp
labo
paper
snap
stock
vsj
Powered by hns-2.19.5, HyperNikkiSystem Project

ÃæÌîÉðͺ (NAKANO, Takeo) <nakano@st.seikei.ac.jp> Since 1999-10-07
RSS feed, ¹¹¿·»þ¹ï, LIRS ¥¨¥ó¥È¥ê, ¥¢¥¯¥»¥¹À©¸æ (²òÀâ)

ÃæÌî¤Î¥Û¡¼¥à¥Ú¡¼¥¸¤Ø