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¡÷ Band bending and the thermochemistry of oxygen vacancies in ionic metal oxide thin films:

oxide Ãæ¤Î»ÀÁÇ vacancy ¤È ambient oxygen ¤Î´Ö¤ÎÊ¿¹Õ¤ÎÏᣠoxygen vacancy ¤Î defect state ¤è¤ê¤â fermi level ¤¬²¼¤Ê¶â°¥³¥ó¥¿¥¯¥È¤Ë¤è¤Ã¤Æ¡¢ band bend¢ªelectron escape ¤¬À¸¤¸¤Æ¤³¤ÎÊ¿¹Õ¤¬¤º¤ì¤ë¡¢¤È¤¤¤¦Äó°Æ¡£ ¼ÂºÝ¤Ë HfO2 ¤Î¾ì¹ç¤òÂоݤˤ·¤¿¼Â¸³¤Ç¡¢ free energy ¤¬ bulk ¤Î¤½¤ì¤è¤ê¤â¤«¤Ê¤êÄ㤯¤Ê¤ë·ë²Ì¤¬¤¢¤ë¤½¤¦¤Ç¡¢ ¤½¤¤¤Ä¤Î¥á¥«¥Ë¥º¥à¤Ç¤Ï¤Ê¤¤¤«¡¢¤È¤Î¤³¤È¡£

¡÷ Spatially localized one-dimensional porous silicon photonic crystals:

p ·¿ Si ¤ËÅÅή̩ÅÙ¤òÁý¸º¤µ¤»¤Æ PS ¤Î 1D ¥Õ¥©¥È¥Ë¥Ã¥¯·ë¾½ (PC) ¤òºî¤ê¡¢ ¤½¤ì¤Î°ìÉô¤Ë¸÷¤ò¾È¼Í¤µ¤»¤¿¤Î¤Á¤Ë¥á¥¿¥Î¡¼¥ë¤ËÄÒ¤±¤ë¤È¡¢ ¸÷¤òÅö¤Æ¤¿¤È¤³¤í¤Ï»À²½¤·¤Æ PC ¤¬°Ý»ý¤µ¤ì¡¢ ¤½¤ì°Ê³°¤Î¤È¤³¤í¤Ï PC ¤¬²õ¤ì¤ë¡¢¤È¤¤¤¦Ïá£

¡÷ Memory effect in argon in the presence of vacuum and gas electrical breakdown mechanisms:

Ar 0.4 Pa ¤Ç¤ÎÊüÅÅÇ˲õ¤¬¡¢gas ͳÍè¤Î¤â¤Î¤«ÅŶËͳÍè¤Î¤â¤Î¤«¤òɾ²Á¤·¤¿Ïᣠgap ŤòÊѤ¨¤Ä¤Ä¡¢ÊüÅÅÅÅ°µ°õ²Ã¤Î interval ¤òÊѤ¨¤Ä¤Ä¡¢ ÊüÅŤÎΩ¤Á¾å¤¬¤ê¤ò¸«¤ë¤Èξ¼Ô¤¬¶èÊ̤Ǥ­¤ë¡¢¤È¤¤¤¦¤³¤È¤é¤·¤¤¡£

¡÷ Three-dimensional crystalline Si film growth by the Ni silicide mediation:

SiO2 ¤Î¾å¤Ë Ni Ëì¤òÄ¥¤Ã¤Æ¡¢¤½¤Î¾å¤Ë Si ¤ò DC ¥¹¥Ñ¥Ã¥¿¤¹¤ë¤È¡¢ ¥¢¥â¥ë¥Õ¥¡¥¹¤¸¤ã¤Ê¤¯¤Æ·ë¾½¤Î Si ¤¬¤Ç¤­¤ë¤È¤¤¤¦Ïᣠ¹â¸úΨ¤ÎÂÀÍÛÅÅÃӤؤÎŬÍÑÎ㤬¡£ ÃÇÌÌ TEM ¤Ç¡¢À®Ä¹²áÄø¤Ê¤É¤¬¹Í»¡¤µ¤ì¤Æ¤¤¤ë¡£ ¤Ê¤ó¤Ç¤½¤¦¤Ê¤ë¤Î¤«¤ÏÎɤ¯¤ï¤«¤é¤ó¤¬¡£

¡÷ Valence band structure of AlN probed by photoluminescence:

¥µ¥Õ¥¡¥¤¥¢´ðÈľå¤Ë MOCVD ¤Ç·ç´Ù¤Î¾¯¤Ê¤¤ c ¼´ÇÛ¸þ¤Î AlN Ëì (4um) ¤òºî¤ê¡¢ p/s Êѹ¹¤Î deep UV Î嵯¸÷¤òÅö¤Æ¡¢PL ¤«¤é¦£ÅÀ¼þ¤ê¤Î VB ¤Î½ç°Ì¤ò¬¤Ã¤¿Ïᣠ¶ñÂÎŪ¤Ë¤Ï top ¤Î 199meV ²¼¡¢¤µ¤é¤Ë¤½¤Î 13meV ²¼¤Ë½ç°Ì¤¬¤¢¤ë¤Ç¡¢¤È¤Î¤³¤È¡£ ÍýÏÀÃͤÈÈæ³Ó¤·¤Æ¤¤¤¿¤ê¡£

¡÷ Extractable, elevated ion charge states in the transition regime from vacuum sparks to high current vacuum arcs:

Anders ÀèÀ¸¤Î¤È¤³¤í¡£¥¢¡¼¥¯¤ÎÁõÃÖ¤ÎÅŸ»¤ò 11uF ¤Î¥³¥ó¥Ç¥ó¥µ¤Ë¤·¤Æ¡¢ 4kV ¤Þ¤Ç¤ÎÃßÅÅ¤Ç max 10kA 8us ¤Î¥Ñ¥ë¥¹ÊüÅÅ (vacuum spark ¤È¤¤¤¦¤½¤¦¤Ê) ¤ò¤µ¤»¡¢TOF ¤Ç (¥¢¡¼¥¯¤è¤ê²Á¿ô¤Î¿¤¤) ¿²Á¥¤¥ª¥ó¤ÎȯÀ¸¤ò³Îǧ¤·¤¿¡¢¤È¤¤¤¦Ïá£

¡÷ Stability of p-type conductivity in nitrogen-doped ZnO thin film:

Zn oxynitride ¤Î thermal oxidation ¤Çºî¤Ã¤¿ N ¥É¡¼¥×¤Î p ·¿ ZnO ¤¬¡¢ °Å½ê¤Ç¤Ï 1 ǯ°Ê¾å Hall ¬Äê¤Ç p ·¿¤ò¼¨¤·Â³¤±¤ë¤¬¡¢ 2.7 eV ¤Î photon ¤òÅö¤Æ¤ë¤È n ·¿¤Ë¤Ê¤Ã¤Á¤ã¤¦¤è¡¢¤È¤¤¤¦¼Â¸³¡£ ¤½¤Î¸å¿ô»þ´Ö°Å½ê¤ÇÊüÃÖ¤¹¤ë¤È¡¢½ù¡¹¤Ë p ·¿¤ËÌá¤ë¤È¤Î¤³¤È¡£ ¤¦¡¼¤ó¡£

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#3 ¥Á¥ã¥ê

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#2 [labo] ½¤»ÎȯɽÎý½¬

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#1 [LDP] 2/7 ¤Î updates

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2001ǯ02·î07Æü(¿å) [nǯÆüµ­]

#7 [linux] migrate ¤Î X 4.0.2

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(EE) SAVAGE(0): Failed to fetch any BIOS modes.
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lspci ¤Ç¤Ï
01:00.0 VGA compatible controller: S3 Inc. Savage 4 (rev 04)
¤È½Ð¤ë¤Î¤Ç¡¢savage ¤Ç¤¢¤ë¤³¤È¤Ï´Ö°ã¤¤¤Ê¤¤¤é¤·¤¤¤Î¤Ç¤µ¤é¤Ëõº÷¡£ ¾åµ­¥¨¥é¡¼¥á¥Ã¥»¡¼¥¸¤Ç google ¤È¤« deja ¤È¤«¸¡º÷¤·¤¿¤é¡¢ color depth ¤¬±¾¡¹¡¢¤È¤¤¤¦¥á¥Ã¥»¡¼¥¸¤¬¤¢¤Ã¤¿¤Î¤Ç¡¢ »î¤·¤Ë 16 ¤Ë¤·¤Æ¤ß¤¿¤éµ¯Æ°¡£24, 32 ¤Ï¥À¥á¤é¤·¤¤¡£

°Ê²¼¾®Ìîß·¤µ¤ó¤Ë¾Ò²ð¤·¤Æ¤â¤é¤Ã¤¿ URL ¤ò¤¤¤¯¤Ä¤«¡£ Æó¤Ä¤á¤Ë¤ÏºòÆüÉÕ¤±¤Ç½Ð¤¿ 1.1.12 ¤È¤¤¤¦ savage_drv.o ¤¬¤¢¤Ã¤¿¤Î¤À¤¬¡¢ ¤³¤ì¤â depth 32 ¤Ç¤ÏÆ°¤«¤Ê¤«¤Ã¤¿¡£ »°¤Ä¤á¤Ë¤Ï
Go back to XF3.3.6. The Savage4 doesn't work well in 4.0+. I have a StealthIII S540 and use 3.3.6.
¤È¤¢¤Ã¤¿¤¬¡¢4.0.2 ¤Ç¤ÏÆ°¤¯¤è¤¦¤Ë¤Ê¤Ã¤¿¤ó¤«¤·¤é¤ó¡£ ¤Þ¤¢ gnome-session ¤â rxvt ¤â VJE ¤â̵»öµ¯Æ°¤·¤¿¤Î¤Ç¡¢ ¤È¤ê¤¢¤¨¤º¤³¤ì¤Ç OK¡£´¶¼Õ¡£

#6 [freshmeat] 2/6 ʬ¤Î¿·Ãå¥á¡¼¥ë¤«¤é

#5 [URL] ``Reply-To'' Munging Considered Harmful

Some administrators claim that Reply-To munging makes it easier for users to respond to the entire list, and helps encourage list traffic. These benefits are fallacious. Moreover, Reply-To can have harmful -- even dangerous -- effects. If you think Reply-To munging is a good idea, I hope I can change your mind.

#4 [linux] slatec

new maintainer ¤¬¸½¤ì¤¿¤é¤·¤¤¡£¤ï¡¼¤¤¡£

#3 [labo] Æþ»î´ØÏ¢¶È̳

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#2 [URL] EPO - The Editing Process Organizer

EPO¤Ï¤¢¤é¤æ¤ë¥×¥í¥°¥é¥ß¥ó¥°¸À¸ì/¥Þ¡¼¥¯¥¢¥Ã¥×¸À¸ì¤Ç¤ÎÊÔ½¸ºî¶È¤òÅý°ìŪ ¤Ë»Ù±ç¤·¤Þ¤¹¡£¤¤¤ï¤Ð ¡Ö¤É¤³¤Ç¤âÌîÄ»¡×¤Ê´Ä¶­¤ò¤á¤¶¤·¤Þ¤¹¡£
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#1 [thesis] matlab -> eps ¤Ç¤Î strings

TeX ɽµ­¤Ç \mu ¤È¤« 3\times 10^{-6} ¤È¤«»È¤¨¤ë¤³¤È¤Ë¤Ê¤Ã¤Æ¤¤¤ë¤Î¤À¤¬¡¢ eps ½ÐÎϤ¹¤ë¤È¤½¤ì¤é¤Î¥·¥ó¥Ü¥ë¤ÎÁ°¤Ë¥¹¥Ú¡¼¥¹¤¬Æþ¤Ã¤Æ»È¤¤Êª¤Ë¤Ê¤é¤ó¡£
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2000ǯ02·î07Æü(·î) [nǯÆüµ­]

#5 [paper] º£ÆüÆɤó¤ÀÏÀʸ

JAP 2/1 ¹æ. ¤Ê¤ó¤«Â¿¤«¤Ã¤¿. ɬÍפˤʤ俤顢 ¤ä¤Ã¤Ñ¤ê»æ¤Ë°õºþ¤·¤Æ¤Á¤ã¤ó¤ÈÆɤޤʤ¤¤È¥À¥á¤Ã¤Ý¤¤(;_;)

¡÷ T. Liu, et al.; JAP 87(3) pp.1070 (2000):

A two-dimensional hybrid model for an electron cyclotron resonance (ECR) plasma reactor is improved by taking into account the microwave absorption. With this code, the velocity and angle distribution function of ions in the source and downstream areas, and the ion current density at the substrate surface in an extended ECR plasma reactor were investigated.
±ßÅû·Ï¤Ç Microwave ¤ÎÅż§¾ì¤È¥×¥é¥º¥Þ¤ÎÁê¸ßºîÍѤò¹Í¤¨¡¢ ¥¤¥ª¥óÀ¸À®¤Ê¤É¤Ï Particle-in cell ¤È MC ¤ÎÁȤ߹ç¤ï¤». ¤·¤«¤· detail ¤¬ Chinese ¤Î Dr. thesis ¤È¤ï...

¡÷ R. Prioli, D. C. Reigada and F. L. Freire, Jr.; JAP 87(3) pp.1118 (2000):

Si3N4 ¤Î AFM ¥Á¥Ã¥×¤Ç B4C ¤ò°ú¤Ã¤«¤­¡¢Ë໤±þÅú¤ò¸«¤¿¼Â¸³. ²Ù½Å¡¢ÁÝ°ú®ÅÙ¤ËÂФ¹¤ë°Í¸À­¤Ê¤É. °ú¤ÃÁߤ­¤ò·«¤êÊÖ¤¹¤ÈɽÌ̤¢¤é¤µ¤¬¸º¤Ã¤ÆË໤¤¬¸º¤ë¤È¤ÎµÄÏÀ¤â¡£

¡÷ L. Lai and E. A. Irene; JAP 87(3) pp.1159 (2000):

p-SI/SiO2/Al ¤Ç Fowler-Nordheim ¥×¥í¥Ã¥È¤ò¤È¤ê¡¢ ÅÅ°µ¤ËÂФ¹¤ëÅÅή¤Î¿ÌÆ°¤È³¦Ì̤Τ¢¤é¤µ¤ò´ØÏ¢¤Å¤±¤Æɾ²Á¤¹¤ëÏá£

¡÷ B. Bhushan and C. Dandavate; JAP 87(3) pp.1201 (2000):

¤¤¤í¤¤¤í¤Ê¥³¡¼¥Æ¥£¥ó¥° (¥Ý¥ê¥Þ¡¼, Diamond like Carbon ¤Ê¤É) ¤Î¡ÖÉÕÃåÎϡפò AFM ¤Ç¬¤Ã¤¿ÏÀʸ¡£ Normal Force vs Z piezo ¤Î¹Ô¤­µ¢¤ê¤«¤éÉÕÃåÎϤòɾ²Á¡£¤Õ¤à¡£

¡÷ H. H. Yu and Z. Suo; JAP 87(3) pp.1211 (2000):

±þÎϤÎÆþ¤Ã¤¿É½Ì̤Τ¢¤é¤µ¤Î»þ´ÖȯŸ¤Ë¤Ä¤¤¤ÆµÄÏÀ. ¥¨¥Ã¥Á¥ó¥°Á°¸å¤Î AFM Áü¤Î¥Õ¡¼¥ê¥¨¥¹¥Ú¥¯¥È¥ë¤òÈæ³Ó¤¹¤ëÊýË¡¤¬»È¤¨¤ë¤é¤·¤¤¡£ ɽÌ̸¶»Ò¤Î mobility ¤Î±þÎϰ͸À­¤Ê¤É¤«¤é¡£

¡÷ S. Adachi and N. Takahashi; JAP 87(3) pp.1264 (2000):

reactive DC ¥¹¥Ñ¥Ã¥¿¤Çºî¤Ã¤¿ TiN ¤Îʬ¸÷¥¨¥ê¥×¥½¤ÇͶÅÅΨ¤ÎÇÈŰ͸À­¤òµá¤á¡¢ Drude-Lorentz + ¥Ð¥ó¥É´ÖÁ«°Ü¤ÎÍýÏÀ¼°¤ÈÈæ³Ó¤·¤¿Ïᣠ¥Ð¥ó¥É´ÖÁ«°Ü¤Î¼°¤Ï¤¤¤Ä¤«»²¹Í¤Ë¤Ç¤­¤ë¤«¤Ê¡£

¤Ä¤¤¤Ç¤Ë PRL vol83 ¤ÎºÇ½ª¹æ¤âÆɤࡣ

¡÷ K. Yokoyama, et al; PRL 83(24) pp.5023 (1999):

Si(111)-(­õ3x­õ3) Ag ¤Î non-contact AFM ´Ñ»¡. ¤ª¤ª¡¢¤Á¤ã¤ó¤È Ag ¤Î trimer ¤¬¸«¤¨¤ë¡£

#4 [labo] ±þʪ½Õ

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#3 [JM] º£Æü¤Î commit

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#2 [labo] ESCA ¥¿¡¼¥Ü¥Ý¥ó¥×°Û²»¤Î·ï

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¤Á¤Ê¤ß¤Ë¿¿¶õÅÙ¤Ï 5.4 x 10^-10 Torr. ½çÄ´¤Î¤è¤¦¤À.

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