Acta Physica Sinica - //m.suprmerch.com/ daily 15 2024-11-21 09:34:01 apsoffice@iphy.ac.cn apsoffice@iphy.ac.cn 2024-11-21 09:34:01 zh Copyright ©Acta Physica Sinica All Rights Reserved.  Address: PostCode：100190 Phone: 010-82649829，82649241,82649863 Email: apsoffice@iphy.ac.cn Copyright ©Acta Physica Sinica All Rights Reserved apsoffice@iphy.ac.cn 1000-3290 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.1

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅＧｉｂｂｓ Ａｐｐｅｌｌ (Ｇ Ａ)ｅｑｕａｔｉｏｎｓｆｏｒｖａｒｉａｂｌｅｍａｓｓｈｏｌｏｎｏｍｉｃｓｙｓｔｅｍｓｗｅｒｅｅｓｔａｂｌｉｓｈｅｄ ,ｔｈｅｎｔｈｅｄｅｆｉｎｉｔｉｏｎａｎｄｃｒｉｔｅｒｉｏｎｏｆｔｈｅｆｏｒｍｉｎｖａｒｉａｎｃｅｏｆＧ Ａｅｑｕａｔｉｏｎｓｕｎｄｅｒｔｈｅｉｎｆｉｎｉｔｅｓｉｍａｌｔｒａｎｓｆｏｒｍａｔｉｏｎｓｏｆｇｒｏｕｐｓｗｅｒｅｇｉｖｅｎ .Ｎｅｘｔ,ａｃｏｎ ｓｅｒｖｅｄｑｕａｎｔｉｔｙｃａｎｂｅｄｅｄｕｃｅｄｂｙｕｓｉｎｇｔｈｉｓｆｏｒｍｉｎｖａｒｉａｎｃｅｕｎｄｅｒｃｅｒｔａｉｎｃｏｎｄｉｔｉｏｎｓ,ａｎｄａｎｅｘａｍｐｌｅｗａｓｇｉｖｅｎ


Acta Physica Sinica. 2002 51(1): 1-5. Published 2005-04-11 ]]>

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅＧｉｂｂｓ Ａｐｐｅｌｌ (Ｇ Ａ)ｅｑｕａｔｉｏｎｓｆｏｒｖａｒｉａｂｌｅｍａｓｓｈｏｌｏｎｏｍｉｃｓｙｓｔｅｍｓｗｅｒｅｅｓｔａｂｌｉｓｈｅｄ ,ｔｈｅｎｔｈｅｄｅｆｉｎｉｔｉｏｎａｎｄｃｒｉｔｅｒｉｏｎｏｆｔｈｅｆｏｒｍｉｎｖａｒｉａｎｃｅｏｆＧ Ａｅｑｕａｔｉｏｎｓｕｎｄｅｒｔｈｅｉｎｆｉｎｉｔｅｓｉｍａｌｔｒａｎｓｆｏｒｍａｔｉｏｎｓｏｆｇｒｏｕｐｓｗｅｒｅｇｉｖｅｎ .Ｎｅｘｔ,ａｃｏｎ ｓｅｒｖｅｄｑｕａｎｔｉｔｙｃａｎｂｅｄｅｄｕｃｅｄｂｙｕｓｉｎｇｔｈｉｓｆｏｒｍｉｎｖａｒｉａｎｃｅｕｎｄｅｒｃｅｒｔａｉｎｃｏｎｄｉｔｉｏｎｓ,ａｎｄａｎｅｘａｍｐｌｅｗａｓｇｉｖｅｎ


Acta Physica Sinica. 2002 51(1): 1-5. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 1-5. article doi:10.7498/aps.51.1 10.7498/aps.51.1 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.1 1-5 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.6

Ｉｎｔｈｉｓｐａｐｅｒ,ｉｎａｆｉｒｓｔ ｏｒｄｅｒａｐｐｒｏｘｉｍａｔｉｏｎ ,ｗｅｏｂｔａｉｎｔｈｅｅｆｆｅｃｔｓｏｆｐｅｒｔｕｒｂａｔｉｏｎｓｏｎａｓｔａｔｉｏｎａｒｙｓｏｌｉｔｏｎｆｏｒＴＤＧＬＥ (ｔｉｍｅｄｅｐｅｎｄｅｎｔｇｉｎｚｂｕｒｇ ｌａｎｄａｕｅｑｕａｔｉｏｎ) .Ｎａｍｅｌｙ ,ｗｅｏｂｔａｉｎｔｈｅｓｏｌｉｔｏｎｐａｒａｍｅｔｅｒｖａｒｉａｔｉｏｎａｎｄｔｈｅｇｅｎｅｒａｌｅｘｐｒｅｓｓｉｏｎｏｆｔｈｅｆｉｒｓｔ ｏｒ ｄｅｒｃｏｒｒｅｃｔｉｏｎ .Ａｔｔｈｅｓａｍｅｔｉｍｅ,ｗｅｇｉｖｅｔｈｅｅｘａｃｔｅｘｐｒｅｓｓｉｏｎｏｆａｓｐｅｃｉａｌｅｘａｍｐｌｅ


Acta Physica Sinica. 2002 51(1): 6-9. Published 2005-04-11 ]]>

Ｉｎｔｈｉｓｐａｐｅｒ,ｉｎａｆｉｒｓｔ ｏｒｄｅｒａｐｐｒｏｘｉｍａｔｉｏｎ ,ｗｅｏｂｔａｉｎｔｈｅｅｆｆｅｃｔｓｏｆｐｅｒｔｕｒｂａｔｉｏｎｓｏｎａｓｔａｔｉｏｎａｒｙｓｏｌｉｔｏｎｆｏｒＴＤＧＬＥ (ｔｉｍｅｄｅｐｅｎｄｅｎｔｇｉｎｚｂｕｒｇ ｌａｎｄａｕｅｑｕａｔｉｏｎ) .Ｎａｍｅｌｙ ,ｗｅｏｂｔａｉｎｔｈｅｓｏｌｉｔｏｎｐａｒａｍｅｔｅｒｖａｒｉａｔｉｏｎａｎｄｔｈｅｇｅｎｅｒａｌｅｘｐｒｅｓｓｉｏｎｏｆｔｈｅｆｉｒｓｔ ｏｒ ｄｅｒｃｏｒｒｅｃｔｉｏｎ .Ａｔｔｈｅｓａｍｅｔｉｍｅ,ｗｅｇｉｖｅｔｈｅｅｘａｃｔｅｘｐｒｅｓｓｉｏｎｏｆａｓｐｅｃｉａｌｅｘａｍｐｌｅ


Acta Physica Sinica. 2002 51(1): 6-9. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 6-9. article doi:10.7498/aps.51.6 10.7498/aps.51.6 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.6 6-9 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.10

ＩｎｔｈｉｓｐａｐｅｒｔｈｅＪａｃｏｂｉｅｌｌｉｐｔｉｃｆｕｎｃｔｉｏｎｅｘｐａｎｓｉｏｎｍｅｔｈｏｄｉｓｅｘｔｅｎｄｅｄｔｏｔｈｅｆｉｎｉｔｅｅｘｐａｎｓｉｏｎｆｏｒｔｈｅａｐｐｌｉｅｄＪａｃｏｂｉｃｏｓｉｎｅｅｌｌｉｐｔｉｃｆｕｎｃｔｉｏｎｏｒｔｈｅｔｈｉｒｄｋｉｎｄｏｆＪａｃｏｂｉｅｌｌｉｐｔｉｃｆｕｎｃｔｉｏｎｔｏｃｏｎｓｔｒｕｃｔｔｈｅｎｅｗｐｅｒｉｏｄｉｃｓｏｌｕｔｉｏｎｓｏｆｎｏｎｌｉｎｅａｒｗａｖｅｅｑｕａｔｉｏｎｓ.Ｔｈｅｐｅｒｉｏｄｉｃｓｏｌｕｔｉｏｎｓｏｂｔａｉｎｅｄｂｙｔｈｉｓｍｅｔｈｏｄｃａｎｂｅｒｅｄｕｃｅｄｔｏｔｈｅｓｏｌｉｔａｒｙｗａｖｅｓｏｌｕｔｉｏｎｓｕｎｄｅｒｔｈｅｌｉｍｉｔｃｏｎｄｉｔｉｏｎ.


Acta Physica Sinica. 2002 51(1): 10-14. Published 2005-04-11 ]]>

ＩｎｔｈｉｓｐａｐｅｒｔｈｅＪａｃｏｂｉｅｌｌｉｐｔｉｃｆｕｎｃｔｉｏｎｅｘｐａｎｓｉｏｎｍｅｔｈｏｄｉｓｅｘｔｅｎｄｅｄｔｏｔｈｅｆｉｎｉｔｅｅｘｐａｎｓｉｏｎｆｏｒｔｈｅａｐｐｌｉｅｄＪａｃｏｂｉｃｏｓｉｎｅｅｌｌｉｐｔｉｃｆｕｎｃｔｉｏｎｏｒｔｈｅｔｈｉｒｄｋｉｎｄｏｆＪａｃｏｂｉｅｌｌｉｐｔｉｃｆｕｎｃｔｉｏｎｔｏｃｏｎｓｔｒｕｃｔｔｈｅｎｅｗｐｅｒｉｏｄｉｃｓｏｌｕｔｉｏｎｓｏｆｎｏｎｌｉｎｅａｒｗａｖｅｅｑｕａｔｉｏｎｓ.Ｔｈｅｐｅｒｉｏｄｉｃｓｏｌｕｔｉｏｎｓｏｂｔａｉｎｅｄｂｙｔｈｉｓｍｅｔｈｏｄｃａｎｂｅｒｅｄｕｃｅｄｔｏｔｈｅｓｏｌｉｔａｒｙｗａｖｅｓｏｌｕｔｉｏｎｓｕｎｄｅｒｔｈｅｌｉｍｉｔｃｏｎｄｉｔｉｏｎ.


Acta Physica Sinica. 2002 51(1): 10-14. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 10-14. article doi:10.7498/aps.51.10 10.7498/aps.51.10 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.10 10-14 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.15

Ｑｕａｎｔｕｍｅｒｒｏｒｃｏｒｒｅｃｔｉｏｎｃｏｄｉｎｇｔｅｃｈｎｏｌｏｇｙｉｓｏｆｇｒｅａｔｉｍｐｏｒｔａｎｃｅｆｏｒｑｕａｎｔｕｍｃｏｍｍｕｎｉｃａｔｉｏｎａｓｗｅｌｌａｓｑｕａｎｔｕｍｃｏｍｐｕｔａ ｔｉｏｎ .Ｎｅａｒｌｙａｌｌｏｆｔｈｅｃｌａｓｓｉｃａｌｅｒｒｏｒｃｏｒｒｅｃｔｉｏｎｃｏｄｉｎｇｓｃｈｅｍｅｓｈａｖｅ ,ｆｏｒｔｈｅｔｉｍｅｂｅｉｎｇ,ｂｅｅｎｔｒａｎｓｐｌａｎｔｅｄｔｏｔｈｅｄｏｍａｉｎｏｆｑｕａｎｔｕｍｉｎｆｏｒｍａｔｉｏｎ ;ｎｅｖｅｒｔｈｅｌｅｓｓ,ｔｈｅｍｏｓｔｏｕｔｓｔａｎｄｉｎｇｓｃｈｅｍｅｉｎｃｌａｓｓｉｃａｌｃｏｄｉｎｇｒｅｇｉｏｎ ,ｔｕｒｂｏｃｏｄｅ ,ｓｔｉｌｌｌａｃｋｓｔｈｅｑｕａｎｔｕｍａｎａｌｏ ｇｙｔｉｌｌｎｏｗ .Ｗｅｈａｖｅｃｏｍｐｌｅｔｅｄａｓｉｍｐｌｅｓｃｈｅｍｅｏｆｑｕａｎｔｕｍｒｅｃｕｒｓｉｖｅｓｙｓｔｅｍａｔｉｃｃｏｎｖｏｌｕｔｉｏｎａｌｃｏｄｅｂｙｍｅａｎｓｏｆｑｕａｎｔｕｍｒｅｇｉｓｔｅｒｎｅｔｗｏｒｋ .Ａｔｔｈｅｓａｍｅｔｉｍｅ,ａｋｉｎｄｏｆｅｆｆｉｃｉｅｎｔｑｕａｎｔｕｍｉｎｔｅｒｗｅａｖｅｒｉｓｃｏｎｓｔｒｕｃｔｅｄｕｓｉｎｇｏｎｌｙｑｕａｎｔｕｍＳＷＡＰｇａｔｅｓ.ＡｌｓｏａｓｅｒｉａｌｌｙｃｏｎｃａｔｅｎａｔｅｄｑｕａｎｔｕｍＴｕｒｂｏｃｏｄｅｉｓｄｅｖｅｌｏｐｅｄｂｙａｎａｌｏｇｙｔｏｔｈｅｃｌａｓｓｉｃａｌＴｕｒｂｏｃｏｄｅ .Ａｓｌｉｍｉｔｅｄｂｙｔｈｅｑｕａｎｔｕｍｎｏｎ -ｃｌｏｎｉｎｇｔｈｅｏｒｅｍ ,ｔｈｅｐｒｏｐｏｓｅｄｑｕａｎｔｕｍｔｕｒｂｏｃｏｄｅｉｓｓｅｒｉａｌｌｙｃｏｎｃａｔｅｎａｔｅｄ .Ｑｕａｎｔｕｍｔｕｒｂｏｃｏｄｅｍａｙｎｏｔｏｎｌｙｅｘｔｅｎｄｔｈｅｒｅｓｅａｒｃｈａｒｅａｏｆｑｕａｎｔｕｍｅｒｒｏｒｃｏｒｒｅｃｔｉｏｎｃｏｄｉｎｇｔｅｃｈｎｏｌｏｇｙ,ｂｕｔａｌｓｏｓｏｌｖｅｔｈｅｐｕｚｚｌｅｉｎｃｌａｓｓｉｃａｌｃｏｄｉｎｇｔｈｅｏｒｙ.


Acta Physica Sinica. 2002 51(1): 15-20. Published 2005-04-11 ]]>

Ｑｕａｎｔｕｍｅｒｒｏｒｃｏｒｒｅｃｔｉｏｎｃｏｄｉｎｇｔｅｃｈｎｏｌｏｇｙｉｓｏｆｇｒｅａｔｉｍｐｏｒｔａｎｃｅｆｏｒｑｕａｎｔｕｍｃｏｍｍｕｎｉｃａｔｉｏｎａｓｗｅｌｌａｓｑｕａｎｔｕｍｃｏｍｐｕｔａ ｔｉｏｎ .Ｎｅａｒｌｙａｌｌｏｆｔｈｅｃｌａｓｓｉｃａｌｅｒｒｏｒｃｏｒｒｅｃｔｉｏｎｃｏｄｉｎｇｓｃｈｅｍｅｓｈａｖｅ ,ｆｏｒｔｈｅｔｉｍｅｂｅｉｎｇ,ｂｅｅｎｔｒａｎｓｐｌａｎｔｅｄｔｏｔｈｅｄｏｍａｉｎｏｆｑｕａｎｔｕｍｉｎｆｏｒｍａｔｉｏｎ ;ｎｅｖｅｒｔｈｅｌｅｓｓ,ｔｈｅｍｏｓｔｏｕｔｓｔａｎｄｉｎｇｓｃｈｅｍｅｉｎｃｌａｓｓｉｃａｌｃｏｄｉｎｇｒｅｇｉｏｎ ,ｔｕｒｂｏｃｏｄｅ ,ｓｔｉｌｌｌａｃｋｓｔｈｅｑｕａｎｔｕｍａｎａｌｏ ｇｙｔｉｌｌｎｏｗ .Ｗｅｈａｖｅｃｏｍｐｌｅｔｅｄａｓｉｍｐｌｅｓｃｈｅｍｅｏｆｑｕａｎｔｕｍｒｅｃｕｒｓｉｖｅｓｙｓｔｅｍａｔｉｃｃｏｎｖｏｌｕｔｉｏｎａｌｃｏｄｅｂｙｍｅａｎｓｏｆｑｕａｎｔｕｍｒｅｇｉｓｔｅｒｎｅｔｗｏｒｋ .Ａｔｔｈｅｓａｍｅｔｉｍｅ,ａｋｉｎｄｏｆｅｆｆｉｃｉｅｎｔｑｕａｎｔｕｍｉｎｔｅｒｗｅａｖｅｒｉｓｃｏｎｓｔｒｕｃｔｅｄｕｓｉｎｇｏｎｌｙｑｕａｎｔｕｍＳＷＡＰｇａｔｅｓ.ＡｌｓｏａｓｅｒｉａｌｌｙｃｏｎｃａｔｅｎａｔｅｄｑｕａｎｔｕｍＴｕｒｂｏｃｏｄｅｉｓｄｅｖｅｌｏｐｅｄｂｙａｎａｌｏｇｙｔｏｔｈｅｃｌａｓｓｉｃａｌＴｕｒｂｏｃｏｄｅ .Ａｓｌｉｍｉｔｅｄｂｙｔｈｅｑｕａｎｔｕｍｎｏｎ -ｃｌｏｎｉｎｇｔｈｅｏｒｅｍ ,ｔｈｅｐｒｏｐｏｓｅｄｑｕａｎｔｕｍｔｕｒｂｏｃｏｄｅｉｓｓｅｒｉａｌｌｙｃｏｎｃａｔｅｎａｔｅｄ .Ｑｕａｎｔｕｍｔｕｒｂｏｃｏｄｅｍａｙｎｏｔｏｎｌｙｅｘｔｅｎｄｔｈｅｒｅｓｅａｒｃｈａｒｅａｏｆｑｕａｎｔｕｍｅｒｒｏｒｃｏｒｒｅｃｔｉｏｎｃｏｄｉｎｇｔｅｃｈｎｏｌｏｇｙ,ｂｕｔａｌｓｏｓｏｌｖｅｔｈｅｐｕｚｚｌｅｉｎｃｌａｓｓｉｃａｌｃｏｄｉｎｇｔｈｅｏｒｙ.


Acta Physica Sinica. 2002 51(1): 15-20. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 15-20. article doi:10.7498/aps.51.15 10.7498/aps.51.15 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.15 15-20 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.21

Ｂｙｕｓｉｎｇｔｈｅｍｅｔｈｏｄｏｆｑｕａｎｔｕｍｓｔａｔｉｓｔｉｃｓ,ｗｅｄｉｒｅｃｔｌｙｄｅｒｉｖｅｔｈｅｐａｒｔｉｔｉｏｎｆｕｎｃｔｉｏｎｏｆｔｈｅｂｏｓｏｎｉｃａｎｄｅｒｍｉｏｎｉｃｆｉｅｌｄｏｎｂｌａｃｋｐｌａｎｅａｎｄｏｂｔａｉｎｔｈｅｉｎｔｅｇｒａｌｅｘｐｒｅｓｓｉｏｎｏｆｔｈｅｂｌａｃｋｐｌａｎｅ’ｓｅｎｔｒｏｐｙ,ｗｈｉｃｈａｖｏｉｄｓｔｈｅｄｉｆｆｉｃｕｌｔｙｉｎｓｏｌｖｉｎｇｔｈｅｗａｖｅｅｑｕａｔｉｏｎｏｆｖａｒｉｏｕｓｐａｒｔｉｃｌｅｓ.Ｔｈｅｎｖｉａｔｈｅｉｍｐｒｏｖｅｄｂｒｉｃｋ -ｗａｌｌｍｅｔｈｏｄ,ｍｅｍｂｒａｎｅｍｏｄｅｌ,ｗｅｃａｌｃｕｌａｔｅｔｈｅｂｌａｃｋｐｌａｎｅ’ｓｅｎｔｒｏｐｙａｎｄｆｉｎｄｏｕｔｔｈａｔｉｆｗｅｌｅｔｔｈｅｉｎｔｅｇｒａｌｕｐｐｅｒａｎｄｌｏｗｅｒｌｉｍｉｔｓｂｏｔｈｔｅｎｄｔｏｔｈｅｈｏｒｉｚｏｎ ,ｔｈｅｅｎｔｒｏｐｙｏｆｔｈｅｂｌａｃｋｐｌａｎｅｉｓｐｒｏｐｏｒｔｉｏｎａｌｔｏｔｈｅａｒｅａｏｆｈｏｒｉｚｏｎ.Ｉｎｏｕｒｒｅｓｕｌｔ,ｔｈｅｓｔｒｉｐｐｅｄｔｅｒｍａｎｄｔｈｅｄｉｖｅｒｇｅｎｔｌｏｇａｒｉｔｈｍｉｃｔｅｒｍｉｎｔｈｅｏｒｉｇｉｎａｌｂｒｉｃｋ -ｗａｌｌｍｅｔｈｏｄｎｏｌｏｎｇｅｒｅｘｉｓｔ.Ｉｎｔｈｅｗｈｏｌｅｐｒｏｃｅｓｓ,ｗｅｄｏｎｏｔｔａｋｅａｎｙａｐｐｒｏｘｉｍａｔｉｏｎ .Ｗｅｏｆｆｅｒａｎｅｗｓｉｍｐｌｅａｎｄｄｉｒｅｃｔｗａｙｏｆｃａｌｃｕｌａｔｉｎｇｔｈｅｅｎｔｒｏｐｙｏｆｄｉｆｆｅｒｅｎｔｃｏｍｐｌｉｃａｔｅｄｂｌａｃｋｈｏｌｅｓ.


Acta Physica Sinica. 2002 51(1): 21-24. Published 2005-04-11 ]]>

Ｂｙｕｓｉｎｇｔｈｅｍｅｔｈｏｄｏｆｑｕａｎｔｕｍｓｔａｔｉｓｔｉｃｓ,ｗｅｄｉｒｅｃｔｌｙｄｅｒｉｖｅｔｈｅｐａｒｔｉｔｉｏｎｆｕｎｃｔｉｏｎｏｆｔｈｅｂｏｓｏｎｉｃａｎｄｅｒｍｉｏｎｉｃｆｉｅｌｄｏｎｂｌａｃｋｐｌａｎｅａｎｄｏｂｔａｉｎｔｈｅｉｎｔｅｇｒａｌｅｘｐｒｅｓｓｉｏｎｏｆｔｈｅｂｌａｃｋｐｌａｎｅ’ｓｅｎｔｒｏｐｙ,ｗｈｉｃｈａｖｏｉｄｓｔｈｅｄｉｆｆｉｃｕｌｔｙｉｎｓｏｌｖｉｎｇｔｈｅｗａｖｅｅｑｕａｔｉｏｎｏｆｖａｒｉｏｕｓｐａｒｔｉｃｌｅｓ.Ｔｈｅｎｖｉａｔｈｅｉｍｐｒｏｖｅｄｂｒｉｃｋ -ｗａｌｌｍｅｔｈｏｄ,ｍｅｍｂｒａｎｅｍｏｄｅｌ,ｗｅｃａｌｃｕｌａｔｅｔｈｅｂｌａｃｋｐｌａｎｅ’ｓｅｎｔｒｏｐｙａｎｄｆｉｎｄｏｕｔｔｈａｔｉｆｗｅｌｅｔｔｈｅｉｎｔｅｇｒａｌｕｐｐｅｒａｎｄｌｏｗｅｒｌｉｍｉｔｓｂｏｔｈｔｅｎｄｔｏｔｈｅｈｏｒｉｚｏｎ ,ｔｈｅｅｎｔｒｏｐｙｏｆｔｈｅｂｌａｃｋｐｌａｎｅｉｓｐｒｏｐｏｒｔｉｏｎａｌｔｏｔｈｅａｒｅａｏｆｈｏｒｉｚｏｎ.Ｉｎｏｕｒｒｅｓｕｌｔ,ｔｈｅｓｔｒｉｐｐｅｄｔｅｒｍａｎｄｔｈｅｄｉｖｅｒｇｅｎｔｌｏｇａｒｉｔｈｍｉｃｔｅｒｍｉｎｔｈｅｏｒｉｇｉｎａｌｂｒｉｃｋ -ｗａｌｌｍｅｔｈｏｄｎｏｌｏｎｇｅｒｅｘｉｓｔ.Ｉｎｔｈｅｗｈｏｌｅｐｒｏｃｅｓｓ,ｗｅｄｏｎｏｔｔａｋｅａｎｙａｐｐｒｏｘｉｍａｔｉｏｎ .Ｗｅｏｆｆｅｒａｎｅｗｓｉｍｐｌｅａｎｄｄｉｒｅｃｔｗａｙｏｆｃａｌｃｕｌａｔｉｎｇｔｈｅｅｎｔｒｏｐｙｏｆｄｉｆｆｅｒｅｎｔｃｏｍｐｌｉｃａｔｅｄｂｌａｃｋｈｏｌｅｓ.


Acta Physica Sinica. 2002 51(1): 21-24. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 21-24. article doi:10.7498/aps.51.21 10.7498/aps.51.21 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.21 21-24 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.25

Ｄｙｎａｍｉｃｄｅｓｃｒｉｐｔｉｏｎｉｓｇｉｖｅｎｏｆｔｈｅｐｈｅｎｏｍｅｎａｏｆｄｒｏｐｌｅｔｃｏｎｄｅｎｓａｔｉｏｎ .Ｔｈｅｃｈａｎｇｅｏｆｔｈｅｃｈｅｍｉｃｌｐｏｌｅｎｔｉａｌｉｓｄｉｓｃｕｓｓｅｄｆｏｒｔｗｏｔｙｐｅｓｏｆｌｉｑｕｉｄｄｒｏｐｌｅｔｓ.ＴｈｅｃｏｎｄｉｔｉｏｎｆｏｒｔｈｅＢｒｏｗｎａｇｇｒｅｇａｔｉｏｎｔｏｏｃｃｕｒｉｓａｌｓｏｏｂｔａｉｎｅｄ .Ｃｏｍｂｉｎｉｎｇａｌｌｔｈｅｓｅｗｉｔｈｔｈｅｄｒｏｐｏｆｆｒａｄｉｕｓ,ｔｈｅｏｐｔｉｍａｌｃｏｍｔａｃｔａｎｇｌｅｃａｎｔｈｅｎｂｅｄｅｔｅｒｍｉｎｅｄ.


Acta Physica Sinica. 2002 51(1): 25-30. Published 2005-04-11 ]]>

Ｄｙｎａｍｉｃｄｅｓｃｒｉｐｔｉｏｎｉｓｇｉｖｅｎｏｆｔｈｅｐｈｅｎｏｍｅｎａｏｆｄｒｏｐｌｅｔｃｏｎｄｅｎｓａｔｉｏｎ .Ｔｈｅｃｈａｎｇｅｏｆｔｈｅｃｈｅｍｉｃｌｐｏｌｅｎｔｉａｌｉｓｄｉｓｃｕｓｓｅｄｆｏｒｔｗｏｔｙｐｅｓｏｆｌｉｑｕｉｄｄｒｏｐｌｅｔｓ.ＴｈｅｃｏｎｄｉｔｉｏｎｆｏｒｔｈｅＢｒｏｗｎａｇｇｒｅｇａｔｉｏｎｔｏｏｃｃｕｒｉｓａｌｓｏｏｂｔａｉｎｅｄ .Ｃｏｍｂｉｎｉｎｇａｌｌｔｈｅｓｅｗｉｔｈｔｈｅｄｒｏｐｏｆｆｒａｄｉｕｓ,ｔｈｅｏｐｔｉｍａｌｃｏｍｔａｃｔａｎｇｌｅｃａｎｔｈｅｎｂｅｄｅｔｅｒｍｉｎｅｄ.


Acta Physica Sinica. 2002 51(1): 25-30. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 25-30. article doi:10.7498/aps.51.25 10.7498/aps.51.25 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.25 25-30 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.31

Ｕｓｉｎｇｔｈｅｄｉｓｔａｎｃｅ ｄｅｐｅｎｄｅｎｔｔｉｇｈｔ ｂｉｎｄｉｎｇｍｏｌｅｃｕｌａｒｄｙｎａｍｉｃｓｍｏｄｅｌ(ＤＤＴＢ ＭＤ) ,ｔｈｅＮａ6 (2Ｄ) +Ｎａ8,Ｎａ6 (3Ｄ) +Ｎａ8ｃｏｌｌｉｓｉｏｎｄｙｎａｍｉｃｐｒｏｃｅｓｓｅｓｈａｖｅｂｅｅｎｓｔｕｄｉｅｄｆｏｒｄｉｆｆｅｒｅｎｔｉｎｃｉｄｅｎｔｅｎｅｒｇｉｅｓａｎｄｄｉｆｆｅｒｅｎｔｉｍｐａｃｔｐａｒａｍｅｔｅｒｓ.Ｄｉｆｆｅｒｅｎｔｒｅａｃｔｉｏｎｍｅｃｈａｎｉｓｍｓｈａｖｅｂｅｅｎｏｂｓｅｒｖｅｄ ,ｓｕｃｈａｓｆｕｓｉｏｎｒｅａｃｔｉｏｎ ,ｄｅｅｐｉｎｅｌａｓｔｉｃａｎｄｑｕａｓｉ ｅｌａｓｔｉｃｃｏｌｌｉｓｉｏｎｓ,ｗｈｉｃｈａｒｅｓｉｍｉｌａｒｔｏｔｈｅｎｕｃｌｅａｒｈｅａｖｙ ｉｏｎｃｏｌｌｉｓｉｏｎｓ.Ｔｈｉｓｓｈｏｗｓｔｈａｔｔｈｅｃｌｕｓｔｅｒｓｗｉｔｈｄｉｆｆｅｒｅｎｔｇｅｏｍｅｔｒｉｃｓｔｒｕｃｔｕｒｅｓｃｏｌｌｉｄｉｎｇｗｉｔｈｉｄｅｎｔｉｃａｌｃｌｕｓｔｅｒｓｃａｎｐｒｏｄｕｃｅｄｉｆｆｅｒｅｎｔｎｅｗｃｌｕｓｔｅｒｓ.Ａｔｌｏｗｅｒｉｎｃｉｄｅｎｔｅｎｅｒｇｙｃｅｎｔｒａｌｃｏｌｌｉｓｉｏｎｓ,Ｎａ6 (3Ｄ)ｃａｎｆｏｒｍａｓｔａｂｌｅｃｌｕｓｔｅｒ;ａｔｌｅＶ ｎｈａｌｆｃｅｎｔｒａｌｃｏｌｌｉｓｉｏｎ ,Ｎａ6 (3Ｄ)ｉｓｅａｓｙｔｏｆｏｒｍａｌａｒｇｅｒｃｌｕｓｔｅｒ.


Acta Physica Sinica. 2002 51(1): 31-35. Published 2005-04-11 ]]>

Ｕｓｉｎｇｔｈｅｄｉｓｔａｎｃｅ ｄｅｐｅｎｄｅｎｔｔｉｇｈｔ ｂｉｎｄｉｎｇｍｏｌｅｃｕｌａｒｄｙｎａｍｉｃｓｍｏｄｅｌ(ＤＤＴＢ ＭＤ) ,ｔｈｅＮａ6 (2Ｄ) +Ｎａ8,Ｎａ6 (3Ｄ) +Ｎａ8ｃｏｌｌｉｓｉｏｎｄｙｎａｍｉｃｐｒｏｃｅｓｓｅｓｈａｖｅｂｅｅｎｓｔｕｄｉｅｄｆｏｒｄｉｆｆｅｒｅｎｔｉｎｃｉｄｅｎｔｅｎｅｒｇｉｅｓａｎｄｄｉｆｆｅｒｅｎｔｉｍｐａｃｔｐａｒａｍｅｔｅｒｓ.Ｄｉｆｆｅｒｅｎｔｒｅａｃｔｉｏｎｍｅｃｈａｎｉｓｍｓｈａｖｅｂｅｅｎｏｂｓｅｒｖｅｄ ,ｓｕｃｈａｓｆｕｓｉｏｎｒｅａｃｔｉｏｎ ,ｄｅｅｐｉｎｅｌａｓｔｉｃａｎｄｑｕａｓｉ ｅｌａｓｔｉｃｃｏｌｌｉｓｉｏｎｓ,ｗｈｉｃｈａｒｅｓｉｍｉｌａｒｔｏｔｈｅｎｕｃｌｅａｒｈｅａｖｙ ｉｏｎｃｏｌｌｉｓｉｏｎｓ.Ｔｈｉｓｓｈｏｗｓｔｈａｔｔｈｅｃｌｕｓｔｅｒｓｗｉｔｈｄｉｆｆｅｒｅｎｔｇｅｏｍｅｔｒｉｃｓｔｒｕｃｔｕｒｅｓｃｏｌｌｉｄｉｎｇｗｉｔｈｉｄｅｎｔｉｃａｌｃｌｕｓｔｅｒｓｃａｎｐｒｏｄｕｃｅｄｉｆｆｅｒｅｎｔｎｅｗｃｌｕｓｔｅｒｓ.Ａｔｌｏｗｅｒｉｎｃｉｄｅｎｔｅｎｅｒｇｙｃｅｎｔｒａｌｃｏｌｌｉｓｉｏｎｓ,Ｎａ6 (3Ｄ)ｃａｎｆｏｒｍａｓｔａｂｌｅｃｌｕｓｔｅｒ;ａｔｌｅＶ ｎｈａｌｆｃｅｎｔｒａｌｃｏｌｌｉｓｉｏｎ ,Ｎａ6 (3Ｄ)ｉｓｅａｓｙｔｏｆｏｒｍａｌａｒｇｅｒｃｌｕｓｔｅｒ.


Acta Physica Sinica. 2002 51(1): 31-35. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 31-35. article doi:10.7498/aps.51.31 10.7498/aps.51.31 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.31 31-35 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.36

ＷｅｐｒｅｓｅｎｔａｎｅｗＱｕａｓｉ Λ ｍｏｄｅｌ ｆｏｕｒ ｌｅｖｅｌｓｙｓｔｅｍｂａｓｅｄｏｎａｇｅｎｅｒａｌｔｈｒｅｅ ｌｅｖｅｌΛ ｍｏｄｅｌａｎｄｉｎｖｅｓｔｉｇａｔｅｔｈｅｒｅｓｏｎａｎｔｆｌｕｏｒｅｓｃｅｎｃｅｓｐｅｃｔｒｏｓｃｏｐｙｉｎｄｅｔａｉｌ.Ｔｈｅｒｅａｒｅｔｈｒｅｅｕｌｔｒａ ｎａｒｒｏｗｓｐｅｃｔｒａｌｌｉｎｅｓｉｎｔｈｅｓｐｏｎｔａｎｅｏｕｓｅｍｉｓｓｉｏｎｓｐｅｃｔｒａｆｒｏｍｕｐｐｅｒｌｅｖｅｌｔｏｌｏｗｅｒ ｌｙｉｎｇｌｅｖｅｌｓｏｆｔｈｅｔｗｏｅｍｉｓｓｉｏｎｃｈａｎｎｅｌｓ,ｗｈｉｃｈｏｃｃｕｒｏｖｅｒａｗｉｄｅｒａｎｇｅｏｆｔｈｅｐａｒａｍｅｔｅｒｓ.Ｔｈｅａｐｐｅａｒａｎｃｅｏｆｔｈｅｔｈｒｅｅｕｌｔｒａ ｎａｒｒｏｗｓｐｅｃｔｒａｌｌｉｎｅｓｉｓｃｌｏｓｅｌｙｒｅｌａｔｅｄｗｉｔｈＲａｂｉｆｒｅｑｕｅｎｃｙｏｆｔｈｅｔｗｏｃｏｈｅｒｅｎｃｅｄｒｉｖｉｎｇｆｉｅｌｄｓ;ａｎｄｔｈｅｌａｒｇｅｒｔｈｅＲａｂｉｆｒｅｑｕｅｎｃｙ ,ｔｈｅｎａｒｒｏｗｅｒｔｈｅｌｉｎｅｓ.Ｔｈｅｅｆｆｅｃｔｏｆｌｉｎｅｎａｒｒｏｗｉｎｇｄｏｅｓｎ’ｔｏｃｃｕｒｗｈｅｎｔｈｅｒｅｉｓｏｎｌｙａｃｏｈｅｒｅｎｃｅｄｒｉｖｉｎｇｆｉｅｌｄ .Ｗｈｉｌｅｔｈｅｉｎｃｏｈｅｒｅｎｔｔｒａｎｓｉｔｉｏｎａｎｄｔｈｅｃｏｌｌｉｓｉｏｎａｌｄｅｃａｙｂｅｔｗｅｅｎｔｈｅｅｎｅｒｇｙｌｅｖｅｌｓｄｅｓｔｒｏｙｔｈｅｆｅａｔｕｒｅｏｆｔｈｅｓｐｅｃｔｒａｌｎａｒｒｏｗｉｎｇｗｈｉｃｈｍａｙｂｅｃｏｎｓｉｄｅｒｅｄｔｏｂｅｔｈｅｒｅｓｕｌｔｏｆｔｈｅｍｕｌｔｉ ｃｈａｎｎｅｌｑｕａｎｔｕｍｉｎｔｅｒｆｅｒｅｎｃｅ.


Acta Physica Sinica. 2002 51(1): 36-41. Published 2005-04-11 ]]>

ＷｅｐｒｅｓｅｎｔａｎｅｗＱｕａｓｉ Λ ｍｏｄｅｌ ｆｏｕｒ ｌｅｖｅｌｓｙｓｔｅｍｂａｓｅｄｏｎａｇｅｎｅｒａｌｔｈｒｅｅ ｌｅｖｅｌΛ ｍｏｄｅｌａｎｄｉｎｖｅｓｔｉｇａｔｅｔｈｅｒｅｓｏｎａｎｔｆｌｕｏｒｅｓｃｅｎｃｅｓｐｅｃｔｒｏｓｃｏｐｙｉｎｄｅｔａｉｌ.Ｔｈｅｒｅａｒｅｔｈｒｅｅｕｌｔｒａ ｎａｒｒｏｗｓｐｅｃｔｒａｌｌｉｎｅｓｉｎｔｈｅｓｐｏｎｔａｎｅｏｕｓｅｍｉｓｓｉｏｎｓｐｅｃｔｒａｆｒｏｍｕｐｐｅｒｌｅｖｅｌｔｏｌｏｗｅｒ ｌｙｉｎｇｌｅｖｅｌｓｏｆｔｈｅｔｗｏｅｍｉｓｓｉｏｎｃｈａｎｎｅｌｓ,ｗｈｉｃｈｏｃｃｕｒｏｖｅｒａｗｉｄｅｒａｎｇｅｏｆｔｈｅｐａｒａｍｅｔｅｒｓ.Ｔｈｅａｐｐｅａｒａｎｃｅｏｆｔｈｅｔｈｒｅｅｕｌｔｒａ ｎａｒｒｏｗｓｐｅｃｔｒａｌｌｉｎｅｓｉｓｃｌｏｓｅｌｙｒｅｌａｔｅｄｗｉｔｈＲａｂｉｆｒｅｑｕｅｎｃｙｏｆｔｈｅｔｗｏｃｏｈｅｒｅｎｃｅｄｒｉｖｉｎｇｆｉｅｌｄｓ;ａｎｄｔｈｅｌａｒｇｅｒｔｈｅＲａｂｉｆｒｅｑｕｅｎｃｙ ,ｔｈｅｎａｒｒｏｗｅｒｔｈｅｌｉｎｅｓ.Ｔｈｅｅｆｆｅｃｔｏｆｌｉｎｅｎａｒｒｏｗｉｎｇｄｏｅｓｎ’ｔｏｃｃｕｒｗｈｅｎｔｈｅｒｅｉｓｏｎｌｙａｃｏｈｅｒｅｎｃｅｄｒｉｖｉｎｇｆｉｅｌｄ .Ｗｈｉｌｅｔｈｅｉｎｃｏｈｅｒｅｎｔｔｒａｎｓｉｔｉｏｎａｎｄｔｈｅｃｏｌｌｉｓｉｏｎａｌｄｅｃａｙｂｅｔｗｅｅｎｔｈｅｅｎｅｒｇｙｌｅｖｅｌｓｄｅｓｔｒｏｙｔｈｅｆｅａｔｕｒｅｏｆｔｈｅｓｐｅｃｔｒａｌｎａｒｒｏｗｉｎｇｗｈｉｃｈｍａｙｂｅｃｏｎｓｉｄｅｒｅｄｔｏｂｅｔｈｅｒｅｓｕｌｔｏｆｔｈｅｍｕｌｔｉ ｃｈａｎｎｅｌｑｕａｎｔｕｍｉｎｔｅｒｆｅｒｅｎｃｅ.


Acta Physica Sinica. 2002 51(1): 36-41. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 36-41. article doi:10.7498/aps.51.36 10.7498/aps.51.36 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.36 36-41 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.42

ＷｅｈａｖｅｃａｌｃｕｌａｔｅｄｔｈｅｉｎｔｅｎｓｉｔｙｄｉｓｔｒｉｂｕｔｉｏｎｉｎｔｈｅｆｏｃａｌｒｅｇｉｏｎｏｆａｌａｓｅｒｂｅａｍｗｉｔｈａｓｕｐｅｒＧａｕｓｓｉａｎｐｒｏｆｉｌｅｔｒｕｎｃａｔｅｄｂｙａｃｉｒｃｕｌａｒａｐｅｒｔｕｒｅ.Ｕｓｉｎｇｔｈｅｃａｌｃｕｌａｔｅｄｔｈｅｏｒｅｔｉｃａｌｉｏｎｉｚａｔｉｏｎｖｏｌｕｍｅｖｅｒｓｕｓｔｈｅｌａｓｅｒｉｎｔｅｎｓｉｔｙ ,ｔｈｅｍｕｌｔｉｐｌｅｉｏｎｉｚａｔｉｏｎｙｉｅｌｄｓｏｆａｔｏｍｓｐｒｏｄｕｃｅｄｂｙｔｈｅｔｒｕｎｃａｔｅｄｌａｓｅｒｂｅａｍｉｓｓｔｕｄｉｅｄ .Ａｓａｎｅｘａｍｐｌｅ,ｔｈｅｙｉｅｌｄｓｏｆｍｕｌｔｉｐｌｙｃｈａｒｇｅｄｉｏｎｓｏｆｘｅｎｏｎａｒｅｃａｌｃｕｌａｔ ｅｄｆｏｒｆｏｃｕｓｅｄｉｎｔｅｎｓｉｔｉｅｓｉｎｔｈｅｒａｎｇｅｏｆ1 0 1 3 ｔｏ 1 0 1 6 Ｗ ｃｍ2 .ＯｓｃｉｌｌａｔｉｏｎｓａｎｄｓｕｐｐｒｅｓｓｉｏｎｓｉｎｔｈｅｙｉｅｌｄｃｕｒｖｅｓｂｅｃｏｍｅｏｂｖｉｏｕｓｌｙｗｉｔｈｔｈｅｉｎｃｒｅａｓｅｏｆｔｈｅｔｒｕｎｃａｔｉｏｎｓｏｆａｓｕｐｐｅｒＧａｕｓｓｉａｎｂｅａｍ .Ｆｏｒａｌａｒｇｅｎ,ｓｕｃｈａｓｎ >2 ,ｏｒｆｏｒｓｔｒｏｎｇｔｒｕｎｃａｔｉｏｎｓ,ｓｕｃｈａｓρａ=1 ,ｏｆｔｈｅｓｕｐｐｅｒＧａｕｓｓｉａｎｂｅａｍ ,ｔｈｅｓｈａｐｅｏｆｍｕｌｔｉｐｌｅｉｏｎｉｚａｔｉｏｎｙｉｅｌｄｓｓｈｏｗｓｌｅｓｓｄｅｐｅｎｄｅｎｃｅｏｎｎ.Ｔｈｅｓｅｏｓｃｉｌｌａｔｉｏｎｓａｎｄｓｕｐｐｒｅｓｓｉｏｎｓｉｎｔｈｅｃａｌｃｕｌａｔｅｄｙｉｅｌｄｃｕｒｖｅｓｍａｙｂｅｕｓｅｄｔｏｅｘｐｌａｉｎｔｈｅｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｆｏｒｍｕｌｔｉｐｌｙｃｈａｒｇｅｄｉｏｎｓｏｆｘｅｎｏｎ.


Acta Physica Sinica. 2002 51(1): 42-48. Published 2005-04-11 ]]>

ＷｅｈａｖｅｃａｌｃｕｌａｔｅｄｔｈｅｉｎｔｅｎｓｉｔｙｄｉｓｔｒｉｂｕｔｉｏｎｉｎｔｈｅｆｏｃａｌｒｅｇｉｏｎｏｆａｌａｓｅｒｂｅａｍｗｉｔｈａｓｕｐｅｒＧａｕｓｓｉａｎｐｒｏｆｉｌｅｔｒｕｎｃａｔｅｄｂｙａｃｉｒｃｕｌａｒａｐｅｒｔｕｒｅ.Ｕｓｉｎｇｔｈｅｃａｌｃｕｌａｔｅｄｔｈｅｏｒｅｔｉｃａｌｉｏｎｉｚａｔｉｏｎｖｏｌｕｍｅｖｅｒｓｕｓｔｈｅｌａｓｅｒｉｎｔｅｎｓｉｔｙ ,ｔｈｅｍｕｌｔｉｐｌｅｉｏｎｉｚａｔｉｏｎｙｉｅｌｄｓｏｆａｔｏｍｓｐｒｏｄｕｃｅｄｂｙｔｈｅｔｒｕｎｃａｔｅｄｌａｓｅｒｂｅａｍｉｓｓｔｕｄｉｅｄ .Ａｓａｎｅｘａｍｐｌｅ,ｔｈｅｙｉｅｌｄｓｏｆｍｕｌｔｉｐｌｙｃｈａｒｇｅｄｉｏｎｓｏｆｘｅｎｏｎａｒｅｃａｌｃｕｌａｔ ｅｄｆｏｒｆｏｃｕｓｅｄｉｎｔｅｎｓｉｔｉｅｓｉｎｔｈｅｒａｎｇｅｏｆ1 0 1 3 ｔｏ 1 0 1 6 Ｗ ｃｍ2 .ＯｓｃｉｌｌａｔｉｏｎｓａｎｄｓｕｐｐｒｅｓｓｉｏｎｓｉｎｔｈｅｙｉｅｌｄｃｕｒｖｅｓｂｅｃｏｍｅｏｂｖｉｏｕｓｌｙｗｉｔｈｔｈｅｉｎｃｒｅａｓｅｏｆｔｈｅｔｒｕｎｃａｔｉｏｎｓｏｆａｓｕｐｐｅｒＧａｕｓｓｉａｎｂｅａｍ .Ｆｏｒａｌａｒｇｅｎ,ｓｕｃｈａｓｎ >2 ,ｏｒｆｏｒｓｔｒｏｎｇｔｒｕｎｃａｔｉｏｎｓ,ｓｕｃｈａｓρａ=1 ,ｏｆｔｈｅｓｕｐｐｅｒＧａｕｓｓｉａｎｂｅａｍ ,ｔｈｅｓｈａｐｅｏｆｍｕｌｔｉｐｌｅｉｏｎｉｚａｔｉｏｎｙｉｅｌｄｓｓｈｏｗｓｌｅｓｓｄｅｐｅｎｄｅｎｃｅｏｎｎ.Ｔｈｅｓｅｏｓｃｉｌｌａｔｉｏｎｓａｎｄｓｕｐｐｒｅｓｓｉｏｎｓｉｎｔｈｅｃａｌｃｕｌａｔｅｄｙｉｅｌｄｃｕｒｖｅｓｍａｙｂｅｕｓｅｄｔｏｅｘｐｌａｉｎｔｈｅｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｆｏｒｍｕｌｔｉｐｌｙｃｈａｒｇｅｄｉｏｎｓｏｆｘｅｎｏｎ.


Acta Physica Sinica. 2002 51(1): 42-48. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 42-48. article doi:10.7498/aps.51.42 10.7498/aps.51.42 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.42 42-48 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.49

Ｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｗｉｔｈｄｉｆｆｅｒｅｎｔｄｉａｍｅｔｅｒｓｗｅｒｅｓｙｎｔｈｅｓｉｚｅｄｂｙｍｉｃｒｏｅｍｕｌｓｉｏｎｍｅｔｈｏｄ ,ｉｎｗｈｉｃｈｔｈｅｅｆｆｅｃｔｏｆｔｏｌｕｅｎｅｏｒｃｙｃｌｏｈｅｘａｎｅａｓａｎｏｉｌｐｈａｓｅｏｎｔｈｅｐａｒｔｉｃｌｅｓｉｚｅａｎｄｉｔｓｄｉｓｔｒｉｂｕｔｉｏｎｗａｓｄｅｔｅｃｔｅｄ .Ｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｗｅｒｅｎｅａｒ ｓｐｈｅｒｉｃａｌ,ｂｏｔｈｍｕｌｔｉｃｒｙｓｔａｌｓａｎｄｔｗｉｎｓｗｅｒｅｏｂｓｅｒｖｅｄ.Ｌａｔｔｉｃｅｄｅｆｏｒｍａｔｉｏｎｓｅｘｉｓｔｅｄｉｎｄｉｆｆｅｒｅｎｔｄｅｇｒｅｅｓｂｅｃａｕｓｅｔｈｅｉｎｔｅｒｐｌａｎａｒｓｐａｃｅｄｗａｓｉｎｃｒｅａｓｅｄ.Ｔｈｅｆｌｕｏｒｅｓｃｅｎｃｅｓｐｅｃｔｒａｆｏｒｄｉｆｆｅｒｅｎｔｓｉｚｅｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｄｉｓｐｅｒｓｅｄｉｎｏｒｇａｎｉｃｓｏｌｖｅｎｔｓｗｅｒｅｍｅａｓｕｒｅｄ.Ｔｈｅｒｅａｒｅｔｈｒｅｅｅｍｉｓｓｉｏｎｐｅａｋｓｆｏｒｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓ ｃｈｌｏｒｏｆｏｒｍｓｙｓｔｅｍｓ,ｗｈｉｌｅｎｏｆｌｕｏｒｅｓｃｅｎｃｅｅｍｉｓｓｉｏｎｗａｓｆｏｕｎｄｗｈｅｎｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｄｉｓｐｅｒｓｅｄｉｎｔｏｌｕｅｎｅ .Ｔｈｅｆｌｕｏｒｅｓｃｅｎｃｅｉｎｔｅｎｓｉｔｙｖａｒｉｅｓｗｉｔｈｐａｒｔｉｃｌｅｓｉｚｅｏｆｔｈｅｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓ,ｗｈｉｃｈｏｒｉｇｉｎａｔｅｓｆｒｏｍＡｇ2 ,Ａｇ3 ｃｌｕｓｔｅｒｓｏｎｔｈｅｓｉｌｖｅｒｐａｒｔｉｃｌｅｓｕｒｆａｃｅｐｒｏｄｕｃｅｄｂｙｔｈｅｉｎｔｅｒａｃｔｉｏｎｂｅｔｗｅｅｎｓｉｌｖｅｒａｎｄｃｈｌｏｒｏｆｏｒｍｕｎｄｅｒＵＶｒａｄｉａｔｉｏｎ .Ｔｈｅｒｅａｃｔｉｖｉｔｙａｎｄｔｈｅｎｕｍｂｅｒｏｆｓｕｒｆａｃｅｒｅａｃｔｉｖｅｃｅｎｔｅｒｓｖａｒｙｗｉｔｈｓｉｌｖｅｒｐａｒｔｉｃｌｅｓｉｚｅ,ｒｅｓｕｌｔｉｎｇｉｎｔｈｅｄｉｆｆｅｒｅｎｔｆｌｕｏｒｅｓｃｅｎｃｅｐｈｅｎｏｍｅｎａ.


Acta Physica Sinica. 2002 51(1): 49-54. Published 2005-04-11 ]]>

Ｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｗｉｔｈｄｉｆｆｅｒｅｎｔｄｉａｍｅｔｅｒｓｗｅｒｅｓｙｎｔｈｅｓｉｚｅｄｂｙｍｉｃｒｏｅｍｕｌｓｉｏｎｍｅｔｈｏｄ ,ｉｎｗｈｉｃｈｔｈｅｅｆｆｅｃｔｏｆｔｏｌｕｅｎｅｏｒｃｙｃｌｏｈｅｘａｎｅａｓａｎｏｉｌｐｈａｓｅｏｎｔｈｅｐａｒｔｉｃｌｅｓｉｚｅａｎｄｉｔｓｄｉｓｔｒｉｂｕｔｉｏｎｗａｓｄｅｔｅｃｔｅｄ .Ｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｗｅｒｅｎｅａｒ ｓｐｈｅｒｉｃａｌ,ｂｏｔｈｍｕｌｔｉｃｒｙｓｔａｌｓａｎｄｔｗｉｎｓｗｅｒｅｏｂｓｅｒｖｅｄ.Ｌａｔｔｉｃｅｄｅｆｏｒｍａｔｉｏｎｓｅｘｉｓｔｅｄｉｎｄｉｆｆｅｒｅｎｔｄｅｇｒｅｅｓｂｅｃａｕｓｅｔｈｅｉｎｔｅｒｐｌａｎａｒｓｐａｃｅｄｗａｓｉｎｃｒｅａｓｅｄ.Ｔｈｅｆｌｕｏｒｅｓｃｅｎｃｅｓｐｅｃｔｒａｆｏｒｄｉｆｆｅｒｅｎｔｓｉｚｅｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｄｉｓｐｅｒｓｅｄｉｎｏｒｇａｎｉｃｓｏｌｖｅｎｔｓｗｅｒｅｍｅａｓｕｒｅｄ.Ｔｈｅｒｅａｒｅｔｈｒｅｅｅｍｉｓｓｉｏｎｐｅａｋｓｆｏｒｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓ ｃｈｌｏｒｏｆｏｒｍｓｙｓｔｅｍｓ,ｗｈｉｌｅｎｏｆｌｕｏｒｅｓｃｅｎｃｅｅｍｉｓｓｉｏｎｗａｓｆｏｕｎｄｗｈｅｎｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓｄｉｓｐｅｒｓｅｄｉｎｔｏｌｕｅｎｅ .Ｔｈｅｆｌｕｏｒｅｓｃｅｎｃｅｉｎｔｅｎｓｉｔｙｖａｒｉｅｓｗｉｔｈｐａｒｔｉｃｌｅｓｉｚｅｏｆｔｈｅｓｉｌｖｅｒｎａｎｏｐａｒｔｉｃｌｅｓ,ｗｈｉｃｈｏｒｉｇｉｎａｔｅｓｆｒｏｍＡｇ2 ,Ａｇ3 ｃｌｕｓｔｅｒｓｏｎｔｈｅｓｉｌｖｅｒｐａｒｔｉｃｌｅｓｕｒｆａｃｅｐｒｏｄｕｃｅｄｂｙｔｈｅｉｎｔｅｒａｃｔｉｏｎｂｅｔｗｅｅｎｓｉｌｖｅｒａｎｄｃｈｌｏｒｏｆｏｒｍｕｎｄｅｒＵＶｒａｄｉａｔｉｏｎ .Ｔｈｅｒｅａｃｔｉｖｉｔｙａｎｄｔｈｅｎｕｍｂｅｒｏｆｓｕｒｆａｃｅｒｅａｃｔｉｖｅｃｅｎｔｅｒｓｖａｒｙｗｉｔｈｓｉｌｖｅｒｐａｒｔｉｃｌｅｓｉｚｅ,ｒｅｓｕｌｔｉｎｇｉｎｔｈｅｄｉｆｆｅｒｅｎｔｆｌｕｏｒｅｓｃｅｎｃｅｐｈｅｎｏｍｅｎａ.


Acta Physica Sinica. 2002 51(1): 49-54. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 49-54. article doi:10.7498/aps.51.49 10.7498/aps.51.49 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.49 49-54 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.55

ＴｈｅｙｉｅｌｄｓｏｆＨ~-,Ｈ ,Ｈ_2 ,Ｈ_2~ +ａｎｄＨ_3 ~+ｆｏｒＨ_3~ +ｃｌｕｓｔｅｒｓｐａｓｓｉｎｇｔｈｒｏｕｇｈｃａｒｂｏｎｆｏｉｌｓｈａｖｅｂｅｅｎｍｅａｓｕｒｅｄ .ＴｈｅｒｅｓｕｌｔｓｓｈｏｗｅｄｔｈａｔｔｈｅｃｈａｒｇｅｅｘｃｈａｎｇｅｐｒｏｃｅｓｓｉｎｔｈｅｉｎｔｅｒａｃｔｉｏｎｏｆＨ3 +ｉｏｎｓｗｉｔｈｓｏｌｉｄｓｐｌａｙｓａｋｅｙｒｏｌｅｉｎｔｈｅｆｏｒｍａｔｉｏｎｏｆｔｈｅｓｅｐｒｏｄｕｃｔｓ.ＴｈｅｃｌｕｓｔｅｒｅｆｆｅｃｔｓａｎｄｗａｋｅｅｆｆｅｃｔｓｏｆＨ3 +ｉｏｎｓｉｎｓｏｌｉｄｓａｒｅａｌｓｏｄｉｓｃｕｓｓｅｄｉｎｄｅｔａｉｌ.


Acta Physica Sinica. 2002 51(1): 55-62. Published 2005-04-11 ]]>

ＴｈｅｙｉｅｌｄｓｏｆＨ~-,Ｈ ,Ｈ_2 ,Ｈ_2~ +ａｎｄＨ_3 ~+ｆｏｒＨ_3~ +ｃｌｕｓｔｅｒｓｐａｓｓｉｎｇｔｈｒｏｕｇｈｃａｒｂｏｎｆｏｉｌｓｈａｖｅｂｅｅｎｍｅａｓｕｒｅｄ .ＴｈｅｒｅｓｕｌｔｓｓｈｏｗｅｄｔｈａｔｔｈｅｃｈａｒｇｅｅｘｃｈａｎｇｅｐｒｏｃｅｓｓｉｎｔｈｅｉｎｔｅｒａｃｔｉｏｎｏｆＨ3 +ｉｏｎｓｗｉｔｈｓｏｌｉｄｓｐｌａｙｓａｋｅｙｒｏｌｅｉｎｔｈｅｆｏｒｍａｔｉｏｎｏｆｔｈｅｓｅｐｒｏｄｕｃｔｓ.ＴｈｅｃｌｕｓｔｅｒｅｆｆｅｃｔｓａｎｄｗａｋｅｅｆｆｅｃｔｓｏｆＨ3 +ｉｏｎｓｉｎｓｏｌｉｄｓａｒｅａｌｓｏｄｉｓｃｕｓｓｅｄｉｎｄｅｔａｉｌ.


Acta Physica Sinica. 2002 51(1): 55-62. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 55-62. article doi:10.7498/aps.51.55 10.7498/aps.51.55 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.55 55-62 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.63

Ｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｓｈａｖｅｂｅｅｎｐｒｅｐａｒｅｄｂｙｔｈｅｍｏｌｅｃｕｌａｒｓｅｌｆ ａｓｓｅｍｂｌｙｔｅｃｈｎｉｑｕｅａｎｄｔｈｅｉｒｖｏｌｔａｇｅ ｃｕｒｒｅｎｔｃｈａｒａｃｔｅｒｉｓｔｉｃｓｍｅａｓｕｒｅｄ .Ｏｎｔｈｅｏｔｈｅｒｈａｎｄ,ｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｓｗｅｒｅｓｔｕｄｉｅｄｂｙｔｈｅＭｏｎｔｅＣａｒｌｏｓｉｍｕｌａｔｉｏｎｂａｓｅｄｏｎａｓｅｍｉ ｃｌａｓｓｉｃａｌｔｈｅｏｒｙｏｆｓｉｎｇｌｅｅｌｅｃｔｒｏｎｐｈｅｎｏｍｅｎａ.Ｔｈｅｓｉｍｕｌａｔｄｖｏｌｔａｇｅ ｃｕｒｒｅｎｔｃｕｒｖｅｉｓｓｉｍｉｌａｒｔｏｔｈｅｍｅａｓｕｒｅｄｏｎｅ.Ｔｈｉｓｓｈｏｗｓｔｈａｔｔｈｅａｂｏｖｅｍｅｔｈｏｄｍａｙｂｅｕｓｅｄｔｏｓｔｕｄｙｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｓ.Ｆｕｒｔｈｅｒｍｏｒｅ ,ｔｈｅｓｉｍｕｌａｔｄｒｅｓｕｌｔｓｉｎｄｉｃａｔｅｔｈａｔｔｈｅｖｏｌｔａｇｅ ｃｕｒｒｅｎｔｃｈａｒａｃｔｅｒｉｓｔｉｃｏｆａｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｉｓｄｅｔｅｒｍｉｎｅｄｏｎｌｙｂｙｔｈｅｓｍａｌｌｑｕａｎｔｉｔｙｏｆｎａｎｏｐａｒｔｉｃｌｅｓｉｎｔｈｅｌｏｗｖｏｌｔａｇｅｒｅｇｉｏｎｔｈｏｕｇｈｔｈｅｒｅａｒｅａｌａｒｇｅｎｕｍｂｅｒｏｆｎａｎｏｐａｒｔｉｃｌｅｓｂｅｔｗｅｅｎｔｈｅｔｗｏｅｌｅｃｔｒｏｄｅｓ.


Acta Physica Sinica. 2002 51(1): 63-67. Published 2005-04-11 ]]>

Ｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｓｈａｖｅｂｅｅｎｐｒｅｐａｒｅｄｂｙｔｈｅｍｏｌｅｃｕｌａｒｓｅｌｆ ａｓｓｅｍｂｌｙｔｅｃｈｎｉｑｕｅａｎｄｔｈｅｉｒｖｏｌｔａｇｅ ｃｕｒｒｅｎｔｃｈａｒａｃｔｅｒｉｓｔｉｃｓｍｅａｓｕｒｅｄ .Ｏｎｔｈｅｏｔｈｅｒｈａｎｄ,ｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｓｗｅｒｅｓｔｕｄｉｅｄｂｙｔｈｅＭｏｎｔｅＣａｒｌｏｓｉｍｕｌａｔｉｏｎｂａｓｅｄｏｎａｓｅｍｉ ｃｌａｓｓｉｃａｌｔｈｅｏｒｙｏｆｓｉｎｇｌｅｅｌｅｃｔｒｏｎｐｈｅｎｏｍｅｎａ.Ｔｈｅｓｉｍｕｌａｔｄｖｏｌｔａｇｅ ｃｕｒｒｅｎｔｃｕｒｖｅｉｓｓｉｍｉｌａｒｔｏｔｈｅｍｅａｓｕｒｅｄｏｎｅ.Ｔｈｉｓｓｈｏｗｓｔｈａｔｔｈｅａｂｏｖｅｍｅｔｈｏｄｍａｙｂｅｕｓｅｄｔｏｓｔｕｄｙｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｓ.Ｆｕｒｔｈｅｒｍｏｒｅ ,ｔｈｅｓｉｍｕｌａｔｄｒｅｓｕｌｔｓｉｎｄｉｃａｔｅｔｈａｔｔｈｅｖｏｌｔａｇｅ ｃｕｒｒｅｎｔｃｈａｒａｃｔｅｒｉｓｔｉｃｏｆａｓｉｎｇｌｅｅｌｅｃｔｒｏｎｄｅｖｉｃｅｉｓｄｅｔｅｒｍｉｎｅｄｏｎｌｙｂｙｔｈｅｓｍａｌｌｑｕａｎｔｉｔｙｏｆｎａｎｏｐａｒｔｉｃｌｅｓｉｎｔｈｅｌｏｗｖｏｌｔａｇｅｒｅｇｉｏｎｔｈｏｕｇｈｔｈｅｒｅａｒｅａｌａｒｇｅｎｕｍｂｅｒｏｆｎａｎｏｐａｒｔｉｃｌｅｓｂｅｔｗｅｅｎｔｈｅｔｗｏｅｌｅｃｔｒｏｄｅｓ.


Acta Physica Sinica. 2002 51(1): 63-67. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 63-67. article doi:10.7498/aps.51.63 10.7498/aps.51.63 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.63 63-67 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.68

Ｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅｉｎａｄｉｅｌｅｃｔｒｉｃｇｒａｔｉｎｇｒｅｓｕｌｔｓｆｒｏｍａｒｅｄｉｓｔｒｉｂｕｔｉｏｎｏｆｅｎｅｒｇｙｉｎｐｒｏｐａｇａｔｉｎｇｗａｖｅｓｗｈｅｎｈｉｇｈ ｏｒｄｅｒｓｐａｔｉａｌｈａｒｍｏｎｉｃｓａｒｅｃｏｕｐｌｅｄｔｏｔｈｅｌｅａｋｙｗａｖｅ ｇｕｉｄｅｍｏｄｅｓｓｕｓｔａｉｎｅｄｂｙｔｈｅｇｒａｔｉｎｇ.Ｉｎｔｈｉｓｐａｐｅｒ,ｗｅｈａｖｅａｎａｌｙｚｅｄｔｈｅｇｕｉｄｅｄ ｗａｖｅｍｏｄｅｓｉｎａｗａｖｅｇｕｉｄｅｗｉｔｈａｒｉｇｏｒｏｕｓｃｏｕｐｌｅｄ ｗａｖｅａｐｐｒｏａｃｈ .Ｆｒｏｍｔｈｅａｎａｌｙｚｅｄｒｅｓｕｌｔｓ,ｗｅｈａｖｅｅｓｔｉｍａｔｅｄｐｒｏｐｅｒｌｙｔｈｅｌｏｃａｔｉｏｎｏｆｔｈｅｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅｉｎａｗｅａｋｌｙｍｏｄｕｌａｔｅｄｄｉｅｌｅｃｔｒｉｃｇｒａｔｉｎｇ .Ｗｅａｌｓｏｄｉｓｃｕｓｓｅｄｔｈｅｒｅｌａｔｉｏｎｓａｍｏｎｇｔｈｅｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅ,ｇｒａｔｉｎｇｌａｙｅｒｔｈｉｃｋｎｅｓｓ,ｓｕｂｓｔｒａｔｅｔｈｉｃｋｎｅｓｓ,ａｎｄｔｈｅｉｎｃｉｄｅｎｔａｎｇｌｅ.Ｂｙａｄｏｐｔｉｎｇａｄｅｓｉｇｎｆｏｒａｎｔｉ ｒｅｆｅｃｔｉｏｎ ,ｔｈｅｓｙｍｍｅｔｒｉｃｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅｗｉｔｈｌｏｗｓｉｄｅｂａｎｄｗａｓａｃｈｉｅｖｅｄ .


Acta Physica Sinica. 2002 51(1): 68-73. Published 2005-04-11 ]]>

Ｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅｉｎａｄｉｅｌｅｃｔｒｉｃｇｒａｔｉｎｇｒｅｓｕｌｔｓｆｒｏｍａｒｅｄｉｓｔｒｉｂｕｔｉｏｎｏｆｅｎｅｒｇｙｉｎｐｒｏｐａｇａｔｉｎｇｗａｖｅｓｗｈｅｎｈｉｇｈ ｏｒｄｅｒｓｐａｔｉａｌｈａｒｍｏｎｉｃｓａｒｅｃｏｕｐｌｅｄｔｏｔｈｅｌｅａｋｙｗａｖｅ ｇｕｉｄｅｍｏｄｅｓｓｕｓｔａｉｎｅｄｂｙｔｈｅｇｒａｔｉｎｇ.Ｉｎｔｈｉｓｐａｐｅｒ,ｗｅｈａｖｅａｎａｌｙｚｅｄｔｈｅｇｕｉｄｅｄ ｗａｖｅｍｏｄｅｓｉｎａｗａｖｅｇｕｉｄｅｗｉｔｈａｒｉｇｏｒｏｕｓｃｏｕｐｌｅｄ ｗａｖｅａｐｐｒｏａｃｈ .Ｆｒｏｍｔｈｅａｎａｌｙｚｅｄｒｅｓｕｌｔｓ,ｗｅｈａｖｅｅｓｔｉｍａｔｅｄｐｒｏｐｅｒｌｙｔｈｅｌｏｃａｔｉｏｎｏｆｔｈｅｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅｉｎａｗｅａｋｌｙｍｏｄｕｌａｔｅｄｄｉｅｌｅｃｔｒｉｃｇｒａｔｉｎｇ .Ｗｅａｌｓｏｄｉｓｃｕｓｓｅｄｔｈｅｒｅｌａｔｉｏｎｓａｍｏｎｇｔｈｅｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅ,ｇｒａｔｉｎｇｌａｙｅｒｔｈｉｃｋｎｅｓｓ,ｓｕｂｓｔｒａｔｅｔｈｉｃｋｎｅｓｓ,ａｎｄｔｈｅｉｎｃｉｄｅｎｔａｎｇｌｅ.Ｂｙａｄｏｐｔｉｎｇａｄｅｓｉｇｎｆｏｒａｎｔｉ ｒｅｆｅｃｔｉｏｎ ,ｔｈｅｓｙｍｍｅｔｒｉｃｇｕｉｄｅｄ ｍｏｄｅｒｅｓｏｎａｎｃｅｗｉｔｈｌｏｗｓｉｄｅｂａｎｄｗａｓａｃｈｉｅｖｅｄ .


Acta Physica Sinica. 2002 51(1): 68-73. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 68-73. article doi:10.7498/aps.51.68 10.7498/aps.51.68 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.68 68-73 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.74

ＴｈｅＭｕｅｌｌｅｒｍａｔｒｉｘｓｏｌｕｔｉｏｎｏｆｔｈｅｖｅｃｔｏｒｒａｄｉａｔｉｖｅｔｒａｎｓｆｅｒｅｑｕａｔｉｏｎｗｉｔｈｔｉｍｅｄｅｐｅｎｄｅｎｃｅｉｓｄｅｒｉｖｅｄｉｎｔｈｉｓｐａｐｅｒ.Ｉｔｉｓａｐｐｌｉｅｄｔｏｔｈｅｓｉｍｕｌａｔｉｏｎｏｆｐｏｌａｒｉｍｅｔｒｉｃｂｉｓｔａｔｉｃｓｃａｔｔｅｒｉｎｇｆｒｏｍａｌａｙｅｒｏｆｒａｎｄｏｍｎｏｎ ｓｐｈｅｒｉｃａｌｓｃａｔｔｅｒｅｒｓｎｏｎｕｎｉｆｏｒｍｌｙｏｒｉｅｎｔｅｄｗｈｅｎａＧａｕｓｓｉａｎｐｌａｎｅｐｕｌｓｅｉｓｉｎｃｉｄｅｎｔｕｐｏｎｉｔ.Ｃｏ ｐｏｌａｒｉｚｅｄａｎｄｃｒｏｓｓｐｏｌａｒｉｚｅｄｂｉｓｔａｔｉｃｓｃａｔｔｅｒｉｎｇａｒｅｎｕｍｅｒｉｃａｌｌｙｃａｌｃｕｌａｔｅｄ .Ｔｈｅｐｕｌｓｅｅｃｈｏｅｓａｒｅｃｏｍｐａｒｅｄｗｉｔｈｔｈｅｉｎｃｉｄｅｎｔｐｕｌｓｅ.Ｗｅｄｅｍｏｎｓｔｒａｔｅｔｈｅｆｕｎｃｔｉｏｎａｌｄｅｐｅｎｄｅｎｃｅｏｆｔｈｅｐｕｌｓｅｏｎｔｈｅｐｈｙｓｉｃａｌｐａｒａｍｅｔｅｒｓｏｆａｒａｎｄｏｍｍｅｄｉｕｍ ,ｓｕｃｈａｓｓｐａｔｉａｌｏｒｉｅｎｔａｔｉｏｎａｎｄｆｒａｃｔｉｏｎａｌｖｏｌｕｍｅｏｆｓｃａｔｔｅｒｅｒｓ,ｉｎｃｉｄｅｎｃｅａｎｇｌｅａｎｄｐｏｌａｒｉｚａｔｉｏｎ ,ｔｈｅｌａｙｅｒｄｅｐｔｈｅｔｃ.


Acta Physica Sinica. 2002 51(1): 74-83. Published 2005-04-11 ]]>

ＴｈｅＭｕｅｌｌｅｒｍａｔｒｉｘｓｏｌｕｔｉｏｎｏｆｔｈｅｖｅｃｔｏｒｒａｄｉａｔｉｖｅｔｒａｎｓｆｅｒｅｑｕａｔｉｏｎｗｉｔｈｔｉｍｅｄｅｐｅｎｄｅｎｃｅｉｓｄｅｒｉｖｅｄｉｎｔｈｉｓｐａｐｅｒ.Ｉｔｉｓａｐｐｌｉｅｄｔｏｔｈｅｓｉｍｕｌａｔｉｏｎｏｆｐｏｌａｒｉｍｅｔｒｉｃｂｉｓｔａｔｉｃｓｃａｔｔｅｒｉｎｇｆｒｏｍａｌａｙｅｒｏｆｒａｎｄｏｍｎｏｎ ｓｐｈｅｒｉｃａｌｓｃａｔｔｅｒｅｒｓｎｏｎｕｎｉｆｏｒｍｌｙｏｒｉｅｎｔｅｄｗｈｅｎａＧａｕｓｓｉａｎｐｌａｎｅｐｕｌｓｅｉｓｉｎｃｉｄｅｎｔｕｐｏｎｉｔ.Ｃｏ ｐｏｌａｒｉｚｅｄａｎｄｃｒｏｓｓｐｏｌａｒｉｚｅｄｂｉｓｔａｔｉｃｓｃａｔｔｅｒｉｎｇａｒｅｎｕｍｅｒｉｃａｌｌｙｃａｌｃｕｌａｔｅｄ .Ｔｈｅｐｕｌｓｅｅｃｈｏｅｓａｒｅｃｏｍｐａｒｅｄｗｉｔｈｔｈｅｉｎｃｉｄｅｎｔｐｕｌｓｅ.Ｗｅｄｅｍｏｎｓｔｒａｔｅｔｈｅｆｕｎｃｔｉｏｎａｌｄｅｐｅｎｄｅｎｃｅｏｆｔｈｅｐｕｌｓｅｏｎｔｈｅｐｈｙｓｉｃａｌｐａｒａｍｅｔｅｒｓｏｆａｒａｎｄｏｍｍｅｄｉｕｍ ,ｓｕｃｈａｓｓｐａｔｉａｌｏｒｉｅｎｔａｔｉｏｎａｎｄｆｒａｃｔｉｏｎａｌｖｏｌｕｍｅｏｆｓｃａｔｔｅｒｅｒｓ,ｉｎｃｉｄｅｎｃｅａｎｇｌｅａｎｄｐｏｌａｒｉｚａｔｉｏｎ ,ｔｈｅｌａｙｅｒｄｅｐｔｈｅｔｃ.


Acta Physica Sinica. 2002 51(1): 74-83. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 74-83. article doi:10.7498/aps.51.74 10.7498/aps.51.74 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.74 74-83 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.84

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｓｑｕｅｅｚｉｎｇｅｆｆｅｃｔｓｏｆａｌｉｇｈｔｆｉｅｌｄｉｎｔｈｅＴ ＣｍｏｄｅｌｉｓｓｔｕｄｉｅｄｂｙｍｅａｎｓｏｆｔｈｅｑｕａｎｔｕｍｔｈｅｏｒｙｉｎｔｈｅＣｏｕｎｔｅｒ Ｒｏｔａｔｉｎｇ Ｗａｖｅ Ａｐｐｒｏｘｉｍａｔｉｏｎ (Ｃ ＲＷＡ) .Ｉｔｈａｓｂｅｅｎｓｈｏｗｎｔｈａｔ:ｔｈｅｌｉｔｔｌｅｉｎｄｅｎｔａｔｉｏｎｗｈｉｃｈｒｅｐｒｅｓｅｎｔｓｔｈｅｑｕａｎｔｕｍｎｏｉｓｅｏｆｔｈｅｓｙｓｔｅｍａｐｐｅａｒｓｉｎｔｈｅｅｖｏｌｕｔｉｏｎｃｕｒｖｅｓｏｆＱｕｎｄｅｒｔｈｅＣ ＲＷＡ ;ｔｈｅｑｕａｎｔｕｍｎｏｉｓｅｗｈｉｃｈｉｓｃａｕｓｅｄｂｙｖｉｒｔｕａｌｐｈｏｔｏｎｆｉｅｌｄｇｒａｄｕａｌｌｙｂｅｃｏｍｅｓｗｅａｋｗｈｅｎωｉｎｃｒｅａｓｅｓ;ｔｈｅｑｕａｎｔｕｍｎｏｉｓｅｉｎｃｒｅａｓｅｓｗｈｅｎ ｎｉｎｃｒｅａｓｅｓ;ｔｈｅｖｉｒｔｕａｌｐｈｏｔｏｎｐｒｏｃｅｓｓｃａｎｓｔｒｅｎｇｔｈｅｎｔｈｅｓｑｕｅｅｚｉｎｇｅｆｆｅｃｔｏｂｖｉｏｕｓｌｙ .Ｂｅｓｉｄｅｓ,ｔｈｅｄｅｐｅｎｄｅｎｃｅｏｆｔｈｅａｔｏｍ ｆｉｅｌｄｃｏｕｐｌｉｎｇｃｏｎｓｔａｎｔλａｎｄｔｈｅａｔｏｍ ａｔｏｍｃｏｕｐｌｉｎｇｃｏｎｓｔａｎｔｇｏｎｔｈｅｓｑｕｅｅｚｉｎｇｅｆｆｅｃｔｓｏｆｔｈｅｆｉｅｌｄｉｓｏｂｓｅｒｖｅｄｉｎｏｕｒｒｅｓｕｌｔｓ.


Acta Physica Sinica. 2002 51(1): 84-90. Published 2005-04-11 ]]>

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｓｑｕｅｅｚｉｎｇｅｆｆｅｃｔｓｏｆａｌｉｇｈｔｆｉｅｌｄｉｎｔｈｅＴ ＣｍｏｄｅｌｉｓｓｔｕｄｉｅｄｂｙｍｅａｎｓｏｆｔｈｅｑｕａｎｔｕｍｔｈｅｏｒｙｉｎｔｈｅＣｏｕｎｔｅｒ Ｒｏｔａｔｉｎｇ Ｗａｖｅ Ａｐｐｒｏｘｉｍａｔｉｏｎ (Ｃ ＲＷＡ) .Ｉｔｈａｓｂｅｅｎｓｈｏｗｎｔｈａｔ:ｔｈｅｌｉｔｔｌｅｉｎｄｅｎｔａｔｉｏｎｗｈｉｃｈｒｅｐｒｅｓｅｎｔｓｔｈｅｑｕａｎｔｕｍｎｏｉｓｅｏｆｔｈｅｓｙｓｔｅｍａｐｐｅａｒｓｉｎｔｈｅｅｖｏｌｕｔｉｏｎｃｕｒｖｅｓｏｆＱｕｎｄｅｒｔｈｅＣ ＲＷＡ ;ｔｈｅｑｕａｎｔｕｍｎｏｉｓｅｗｈｉｃｈｉｓｃａｕｓｅｄｂｙｖｉｒｔｕａｌｐｈｏｔｏｎｆｉｅｌｄｇｒａｄｕａｌｌｙｂｅｃｏｍｅｓｗｅａｋｗｈｅｎωｉｎｃｒｅａｓｅｓ;ｔｈｅｑｕａｎｔｕｍｎｏｉｓｅｉｎｃｒｅａｓｅｓｗｈｅｎ ｎｉｎｃｒｅａｓｅｓ;ｔｈｅｖｉｒｔｕａｌｐｈｏｔｏｎｐｒｏｃｅｓｓｃａｎｓｔｒｅｎｇｔｈｅｎｔｈｅｓｑｕｅｅｚｉｎｇｅｆｆｅｃｔｏｂｖｉｏｕｓｌｙ .Ｂｅｓｉｄｅｓ,ｔｈｅｄｅｐｅｎｄｅｎｃｅｏｆｔｈｅａｔｏｍ ｆｉｅｌｄｃｏｕｐｌｉｎｇｃｏｎｓｔａｎｔλａｎｄｔｈｅａｔｏｍ ａｔｏｍｃｏｕｐｌｉｎｇｃｏｎｓｔａｎｔｇｏｎｔｈｅｓｑｕｅｅｚｉｎｇｅｆｆｅｃｔｓｏｆｔｈｅｆｉｅｌｄｉｓｏｂｓｅｒｖｅｄｉｎｏｕｒｒｅｓｕｌｔｓ.


Acta Physica Sinica. 2002 51(1): 84-90. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 84-90. article doi:10.7498/aps.51.84 10.7498/aps.51.84 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.84 84-90 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.91

Ｔｈｅｃｈａｒａｃｔｅｒｉｚａｔｉｏｎｏｆａｌｌ ｏｐｔｉｃａｌｗａｖｅｌｅｎｇｔｈｃｏｎｖｅｒｔｅｒｂａｓｅｄｏｎｔｈｅｃａｓｃａｄｅｄｓｅｃｏｎｄ ｏｒｄｅｒｎｏｎｌｉｎｅａｒｉｔｉｅｓｉｎＬｉＮｂＯ3ｗａｖｅｇｕｉｄｅｓｈａｓｂｅｅｎｃａｒｒｉｅｄｏｕｔｉｎｔｈｉｓｗｏｒｋｉｎｏｒｄｅｒｔｏｆｉｎｄｒｕｌｅｓｔｏｏｐｔｉｍｉｚｅｔｈｅｆａｂｒｉｃａｔｉｏｎｐａｒａｍｅｔｅｒｓｆｏｒｓｔａｂｌｅａｎｄｈｉｇｈ ｅｆｆｉｃｉｅｎｃｙａｌｌ ｏｐｔｉｃａｌｗａｖｅｌｅｎｇｔｈｃｏｎｖｅｎｔｉｏｎ.Ｆｉｒｓｔｌｙ,ｔｈｅｃｏｍｐａｒｉｓｏｎｏｆｎｕｍｅｒｉｃａｌａｎａｌｙｓｉｓｒｅｓｕｌｔｓａｎｄｔｈｅｓｍａｌｌ ｓｉｇｎａｌａｎａｌｙｓｉｓｒｅｓｕｌｔｓｉｓｇｉｖｅｎｂａｓｅｄｏｎｔｈｅｃｏｕｐｌｅｄｍｏｄｅｅｑｕａｔｉｏｎ.Ｓｅｃｏｎｄｌｙ,ｕｓｉｎｇｔｈｅｎｕｍｅｒｉｃａｌｒｅｓｕｌｔｓ,ｔｈｅｄｅｐｅｎｄｅｎｃｅｏｆｔｈｅｆｕｎｄａｍｅｎｔａｌｗａｖｅｌｅｎｇｔｈａｎｄｔｈｅＱＰＭｇｒａｔｉｎｇｐｅｒｉｏｄｏｎｔｈｅｂｕｌｋｔｅｍｐｅｒａｔｕｒｅｉｓｇｉｖｅｎｒｅｓｐｅｃｔｉｖｅｌｙ.Ｆｉｎａｌｌｙ ,ｔｈｅｒｅｌａｔｉｏｎｓｈｉｐｂｅｔｗｅｅｎｔｈｅｏｕｔｐｕｔｐｏｗｅｒｏｆａｃｏｎｖｅｒｔｅｄｌｉｇｈｔａｎｄｔｈｅ 3ｄＢｂａｎｄｗｉｄｔｈｏｆｆｕｎｄａｍｅｎｔａｌｗａｖｅｌｅｎｇｔｈ ,ｂｕｌｋｔｅｍｐｅｒａｔｕｒｅ ,ｇｒａｔｉｎｇｐｅｒｉｏｄｉｓａｎａｌｙｚｅｄ .


Acta Physica Sinica. 2002 51(1): 91-98. Published 2005-04-11 ]]>

Ｔｈｅｃｈａｒａｃｔｅｒｉｚａｔｉｏｎｏｆａｌｌ ｏｐｔｉｃａｌｗａｖｅｌｅｎｇｔｈｃｏｎｖｅｒｔｅｒｂａｓｅｄｏｎｔｈｅｃａｓｃａｄｅｄｓｅｃｏｎｄ ｏｒｄｅｒｎｏｎｌｉｎｅａｒｉｔｉｅｓｉｎＬｉＮｂＯ3ｗａｖｅｇｕｉｄｅｓｈａｓｂｅｅｎｃａｒｒｉｅｄｏｕｔｉｎｔｈｉｓｗｏｒｋｉｎｏｒｄｅｒｔｏｆｉｎｄｒｕｌｅｓｔｏｏｐｔｉｍｉｚｅｔｈｅｆａｂｒｉｃａｔｉｏｎｐａｒａｍｅｔｅｒｓｆｏｒｓｔａｂｌｅａｎｄｈｉｇｈ ｅｆｆｉｃｉｅｎｃｙａｌｌ ｏｐｔｉｃａｌｗａｖｅｌｅｎｇｔｈｃｏｎｖｅｎｔｉｏｎ.Ｆｉｒｓｔｌｙ,ｔｈｅｃｏｍｐａｒｉｓｏｎｏｆｎｕｍｅｒｉｃａｌａｎａｌｙｓｉｓｒｅｓｕｌｔｓａｎｄｔｈｅｓｍａｌｌ ｓｉｇｎａｌａｎａｌｙｓｉｓｒｅｓｕｌｔｓｉｓｇｉｖｅｎｂａｓｅｄｏｎｔｈｅｃｏｕｐｌｅｄｍｏｄｅｅｑｕａｔｉｏｎ.Ｓｅｃｏｎｄｌｙ,ｕｓｉｎｇｔｈｅｎｕｍｅｒｉｃａｌｒｅｓｕｌｔｓ,ｔｈｅｄｅｐｅｎｄｅｎｃｅｏｆｔｈｅｆｕｎｄａｍｅｎｔａｌｗａｖｅｌｅｎｇｔｈａｎｄｔｈｅＱＰＭｇｒａｔｉｎｇｐｅｒｉｏｄｏｎｔｈｅｂｕｌｋｔｅｍｐｅｒａｔｕｒｅｉｓｇｉｖｅｎｒｅｓｐｅｃｔｉｖｅｌｙ.Ｆｉｎａｌｌｙ ,ｔｈｅｒｅｌａｔｉｏｎｓｈｉｐｂｅｔｗｅｅｎｔｈｅｏｕｔｐｕｔｐｏｗｅｒｏｆａｃｏｎｖｅｒｔｅｄｌｉｇｈｔａｎｄｔｈｅ 3ｄＢｂａｎｄｗｉｄｔｈｏｆｆｕｎｄａｍｅｎｔａｌｗａｖｅｌｅｎｇｔｈ ,ｂｕｌｋｔｅｍｐｅｒａｔｕｒｅ ,ｇｒａｔｉｎｇｐｅｒｉｏｄｉｓａｎａｌｙｚｅｄ .


Acta Physica Sinica. 2002 51(1): 91-98. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 91-98. article doi:10.7498/aps.51.91 10.7498/aps.51.91 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.91 91-98 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.99

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｅｘｐｌｉｃｉｔｆｏｒｍｕｌａｏｆＪｏｓｔｆｕｎｃｔｉｏｎｐａｉｒｓｉｎｔｈｅｃａｓｅｏｆｐｕｒｅｒａｄｉａｔｉｏｎｉｓｄｅｒｉｖｅｄｂｙｕｓｉｎｇｔｈｅｄｒｅｓｓｉｎｇｍｅｔｈｏｄａｎｄ,ｔｈｅａｎａｌｙｓｉｓｏｆｔｈｅｉｎｔｅｒａｃｔｉｏｎｂｅｔｗｅｅｎｓｏｌｉｔｏｎｓａｎｄｒａｄｉａｔｉｏｎｉｓｍａｄｅ.Ｉｔｉｓｆｏｕｎｄｔｈａｔｉｎｔｈｅｃｏｕｒｓｅｏｆｔｒａｎｓｍｉｓｓｉｏｎ ,ｔｈｅｏｐｔｉｃａｌｐｕｌｓｅ,ｗｈｏｓｅａｍｐｌｉｔｕｄｅｄｅｃａｙｓａｃｃｏｒｄｉｎｇｔｏｔｈｅｌａｗｏｆｔｈｅｎｅｇａｔｉｖｅｓｑｕａｒｅｒｏｏｔｏｆｐｏｗｅｒｉｎｄｅｘａｌｏｎｇｔｈｅｐｒｏｐａｇａｔｉｎｇｄｉｒｅｃｔｉｏｎ ,ｕｌｔｉｍａｔｅｌｙｅｖｏｌｖｅｓｉｎｔｏｔｈｅｆｏｒｍｏｆｓｏｌｉｔｏｎ ｌｉｋｅｗａｖｅｉｎｔｈｅａｂｓｅｎｃｅｏｆｒａｄｉａｔｉｏｎ .Ｉｔｉｓｒｅｖｅａｌｅｄｔｈａｔｔｈｅｆａｃｔｏｒγｐｌａｙｓａｎｉｍｐｏｒｔａｎｔｒｏｌｅｉｎｔｈｅｓｐｅｃｔｒｕｍｐｒｏｐｅｒｔｉｅｓｆｏｒｔｈｅｏｕｔｐｕｔｏｆｔｈｅｏｐｔｉｃａｌｐｕｌｓｅ .Ｔｈｅｄｙｎａｍｉｃａｌｂｅｈａｖｉｏｕｒｏｆｔｈｅｅｖｏｌｕｔｉｏｎｏｆｓｏｌｉｔｏｎ ｌｉｋｅｗａｖｅｓｄｕｒｉｎｇｔｈｅｉｎｔｅｒａｃｔｉｏｎｏｆｓｏｌｉｔｏｎｓａｎｄｒａｄｉａｔｉｏｎｉｓａｌｓｏａｎａｌｙｚｅｄ.


Acta Physica Sinica. 2002 51(1): 99-103. Published 2005-04-11 ]]>

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｅｘｐｌｉｃｉｔｆｏｒｍｕｌａｏｆＪｏｓｔｆｕｎｃｔｉｏｎｐａｉｒｓｉｎｔｈｅｃａｓｅｏｆｐｕｒｅｒａｄｉａｔｉｏｎｉｓｄｅｒｉｖｅｄｂｙｕｓｉｎｇｔｈｅｄｒｅｓｓｉｎｇｍｅｔｈｏｄａｎｄ,ｔｈｅａｎａｌｙｓｉｓｏｆｔｈｅｉｎｔｅｒａｃｔｉｏｎｂｅｔｗｅｅｎｓｏｌｉｔｏｎｓａｎｄｒａｄｉａｔｉｏｎｉｓｍａｄｅ.Ｉｔｉｓｆｏｕｎｄｔｈａｔｉｎｔｈｅｃｏｕｒｓｅｏｆｔｒａｎｓｍｉｓｓｉｏｎ ,ｔｈｅｏｐｔｉｃａｌｐｕｌｓｅ,ｗｈｏｓｅａｍｐｌｉｔｕｄｅｄｅｃａｙｓａｃｃｏｒｄｉｎｇｔｏｔｈｅｌａｗｏｆｔｈｅｎｅｇａｔｉｖｅｓｑｕａｒｅｒｏｏｔｏｆｐｏｗｅｒｉｎｄｅｘａｌｏｎｇｔｈｅｐｒｏｐａｇａｔｉｎｇｄｉｒｅｃｔｉｏｎ ,ｕｌｔｉｍａｔｅｌｙｅｖｏｌｖｅｓｉｎｔｏｔｈｅｆｏｒｍｏｆｓｏｌｉｔｏｎ ｌｉｋｅｗａｖｅｉｎｔｈｅａｂｓｅｎｃｅｏｆｒａｄｉａｔｉｏｎ .Ｉｔｉｓｒｅｖｅａｌｅｄｔｈａｔｔｈｅｆａｃｔｏｒγｐｌａｙｓａｎｉｍｐｏｒｔａｎｔｒｏｌｅｉｎｔｈｅｓｐｅｃｔｒｕｍｐｒｏｐｅｒｔｉｅｓｆｏｒｔｈｅｏｕｔｐｕｔｏｆｔｈｅｏｐｔｉｃａｌｐｕｌｓｅ .Ｔｈｅｄｙｎａｍｉｃａｌｂｅｈａｖｉｏｕｒｏｆｔｈｅｅｖｏｌｕｔｉｏｎｏｆｓｏｌｉｔｏｎ ｌｉｋｅｗａｖｅｓｄｕｒｉｎｇｔｈｅｉｎｔｅｒａｃｔｉｏｎｏｆｓｏｌｉｔｏｎｓａｎｄｒａｄｉａｔｉｏｎｉｓａｌｓｏａｎａｌｙｚｅｄ.


Acta Physica Sinica. 2002 51(1): 99-103. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 99-103. article doi:10.7498/aps.51.99 10.7498/aps.51.99 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.99 99-103 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.104

Ｓｃｒａｔｃｈ ｒｅｓｉｓｔａｎｔｓｉｌｉｃａａｅｒｏｇｅｌｆｉｌｍｓｗｉｔｈａ 77%ｐｏｒｏｓｉｔｙａｎｄ 1 . 1 2ｒｅｆｒａｃｔｉｖｅｉｎｄｅｘａｔａｍｂｉｅｎｔｐｒｅｓｓｕｒｅｉｓｒｅｐｏｒｔｅｄｕｓｉｎｇｔｈｅｅｘｃｈａｎｇｅｏｆｓｏｌｖｅｎｔａｎｄｍｏｄｉｆｉｃａｔｉｏｎｏｆ—ＣＨ3 ｇｒｏｕｐ.Ｔｈｅｓｉｌｉｃａｆｉｌｍｓｗｅｒｅｐｒｅｐａｒｅｄｉｎａｓｏｌ ｇｅｌｐｒｏｃｅｓｓｂｙａｄｉｐ ｃｏａｔｉｎｇｍｅｔｈｏｄ ,ａｎｄｔｈｅｎｗｅｒｅｐｏｓｔａｎｎｅａｌｅｄｉｎａｉｒａｎｄａｍｉｘｅｄｇａｓａｔｍｏｓｐｈｅｒｅ.Ｔｈｅｆｉｌｍｓｗｅｒｅｃｈａｒａｃｔｅｒｉｚｅｄｗｉｔｈｔｒａｎｓｍｉｓｓｉｏｎｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｅ,ｓｃａｎｎｉｎｇｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｅ,ＦｏｕｒｉｅｒＴｒａｎｓｆｏｒｍｉｎｆｒａｒｅｄｓｐｅｃｔｒｏｓｃｏｐｅ,ａｎｅｌｌｉｐｓｏｍｅｔｅｒ,ａｎｄｔｈｅａｂｒａｓｉｏｎｔｅｓｔ,ｒｅｓｐｅｃｔｉｖｅｌｙ.Ｗｉｔｈｔｈｅｐｏｓｔａｎｎｅａｌｉｎｇ,ｔｈｅｆｒｅｑｕｅｎｃｙｓｈｉｆｔｏｆＦＴＩＲａｂｓｏｒｐｔｉｏｎω4(ＴＯ3 )ｐｅａｋｏｆｔｈｅｆｉｌｍｓｔｏａｌｏｗｅｒｗａｖｅｎｕｍｂｅｒｒｅｓｕｌｔｓｆｒｏｍａｄｅｃｒｅａｓｅｉｎｔｈｅａｖｅｒａｇｅＳｉ—Ｏ—Ｓｉｂｒｉｄｇｉｎｇａｎｇｌｅ.Ａｎｉｎｃｒｅａｓｅｉｎｔｈｅｆｕｌｌｗｉｄｔｈａｔｈａｌｆ ｍａｘｉｍｕｍ (ＦＷＨＭ)ｏｆｔｈｅω4ｐｅａｋｉｓａｓｃｒｉｂｅｄｔｏａｗｉｄｅｄｉｓｔｒｉｂｕｔｉｏｎｏｆｔｈｅｂｒｉｄｇｉｎｇａｎｇｌｅｂｅｃａｕｓｅｏｆｔｈｅｆｏｒｍａｔｉｏｎｏｆｓｔｒａｉｎｅｄＳｉ—Ｏ—Ｓｉｂｏｎｄｓｃａｕｓｅｄｂｙｔｈｅｐｏｓｔａｎｎｅａｌｉｎｇ.Ｔｈｅａｂｒａｓｉｏｎａｎｄａｄｈｅｓｉｏｎｔｅｓｔｓｉｎｄｉｃａｔｅｔｈａｔｔｈｅｍｉｘｅｄｇａｓｔｒｅａｔｍｅｎｔｎｏｔｉｃｅａｂｌｙｓｔｒｅｎｇｔｈｅｎｓｔｈｅｓｉｌｉｃａｎｅｔｗｏｒｋ .ＴｈｅｉｎｃｒｅａｓｅｉｎｓｔｒｅｎｇｔｈｉｓａｔｔｒｉｂｕｔｅｄｔｏｍｏｒｅＳｉ—Ｏ—Ｓｉｂｏｎｄｃｒｏｓｓ ｌｉｎｋａｇｅｓｂｅｔｗｅｅｎｓｉｌｉｃａｐａｒｔｉｃｌｅｓｆｏｒｍｅｄｂｙｔｈｅｍｉｘｅｄｇａｓｔｒｅａｔｍｅｎｔ.


Acta Physica Sinica. 2002 51(1): 104-110. Published 2005-04-11 ]]>

Ｓｃｒａｔｃｈ ｒｅｓｉｓｔａｎｔｓｉｌｉｃａａｅｒｏｇｅｌｆｉｌｍｓｗｉｔｈａ 77%ｐｏｒｏｓｉｔｙａｎｄ 1 . 1 2ｒｅｆｒａｃｔｉｖｅｉｎｄｅｘａｔａｍｂｉｅｎｔｐｒｅｓｓｕｒｅｉｓｒｅｐｏｒｔｅｄｕｓｉｎｇｔｈｅｅｘｃｈａｎｇｅｏｆｓｏｌｖｅｎｔａｎｄｍｏｄｉｆｉｃａｔｉｏｎｏｆ—ＣＨ3 ｇｒｏｕｐ.Ｔｈｅｓｉｌｉｃａｆｉｌｍｓｗｅｒｅｐｒｅｐａｒｅｄｉｎａｓｏｌ ｇｅｌｐｒｏｃｅｓｓｂｙａｄｉｐ ｃｏａｔｉｎｇｍｅｔｈｏｄ ,ａｎｄｔｈｅｎｗｅｒｅｐｏｓｔａｎｎｅａｌｅｄｉｎａｉｒａｎｄａｍｉｘｅｄｇａｓａｔｍｏｓｐｈｅｒｅ.Ｔｈｅｆｉｌｍｓｗｅｒｅｃｈａｒａｃｔｅｒｉｚｅｄｗｉｔｈｔｒａｎｓｍｉｓｓｉｏｎｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｅ,ｓｃａｎｎｉｎｇｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｅ,ＦｏｕｒｉｅｒＴｒａｎｓｆｏｒｍｉｎｆｒａｒｅｄｓｐｅｃｔｒｏｓｃｏｐｅ,ａｎｅｌｌｉｐｓｏｍｅｔｅｒ,ａｎｄｔｈｅａｂｒａｓｉｏｎｔｅｓｔ,ｒｅｓｐｅｃｔｉｖｅｌｙ.Ｗｉｔｈｔｈｅｐｏｓｔａｎｎｅａｌｉｎｇ,ｔｈｅｆｒｅｑｕｅｎｃｙｓｈｉｆｔｏｆＦＴＩＲａｂｓｏｒｐｔｉｏｎω4(ＴＯ3 )ｐｅａｋｏｆｔｈｅｆｉｌｍｓｔｏａｌｏｗｅｒｗａｖｅｎｕｍｂｅｒｒｅｓｕｌｔｓｆｒｏｍａｄｅｃｒｅａｓｅｉｎｔｈｅａｖｅｒａｇｅＳｉ—Ｏ—Ｓｉｂｒｉｄｇｉｎｇａｎｇｌｅ.Ａｎｉｎｃｒｅａｓｅｉｎｔｈｅｆｕｌｌｗｉｄｔｈａｔｈａｌｆ ｍａｘｉｍｕｍ (ＦＷＨＭ)ｏｆｔｈｅω4ｐｅａｋｉｓａｓｃｒｉｂｅｄｔｏａｗｉｄｅｄｉｓｔｒｉｂｕｔｉｏｎｏｆｔｈｅｂｒｉｄｇｉｎｇａｎｇｌｅｂｅｃａｕｓｅｏｆｔｈｅｆｏｒｍａｔｉｏｎｏｆｓｔｒａｉｎｅｄＳｉ—Ｏ—Ｓｉｂｏｎｄｓｃａｕｓｅｄｂｙｔｈｅｐｏｓｔａｎｎｅａｌｉｎｇ.Ｔｈｅａｂｒａｓｉｏｎａｎｄａｄｈｅｓｉｏｎｔｅｓｔｓｉｎｄｉｃａｔｅｔｈａｔｔｈｅｍｉｘｅｄｇａｓｔｒｅａｔｍｅｎｔｎｏｔｉｃｅａｂｌｙｓｔｒｅｎｇｔｈｅｎｓｔｈｅｓｉｌｉｃａｎｅｔｗｏｒｋ .ＴｈｅｉｎｃｒｅａｓｅｉｎｓｔｒｅｎｇｔｈｉｓａｔｔｒｉｂｕｔｅｄｔｏｍｏｒｅＳｉ—Ｏ—Ｓｉｂｏｎｄｃｒｏｓｓ ｌｉｎｋａｇｅｓｂｅｔｗｅｅｎｓｉｌｉｃａｐａｒｔｉｃｌｅｓｆｏｒｍｅｄｂｙｔｈｅｍｉｘｅｄｇａｓｔｒｅａｔｍｅｎｔ.


Acta Physica Sinica. 2002 51(1): 104-110. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 104-110. article doi:10.7498/aps.51.104 10.7498/aps.51.104 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.104 104-110 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.111

Ｔｒａｎｓｉｅｎｔｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙａｎｄｉｔｓｌｉｇｈｔ ｉｎｄｕｃｅｄｃｈａｎｇｅｗｅｒｅｉｎｖｅｓｔｉｇａｔｅｄｂｙｕｓｉｎｇａＭｏｄｅｌ440 0ｂｏｘｃａｒａｖｅｒａｇｅｒａｎｄｓｉｇｎａｌｐｒｏｃｅｓｓｏｒｆｏｒｌｉｇｈｔｌｙｂｏｒｏｎ ｄｏｐｅｄａ Ｓｉ∶Ｈｆｉｌｍｓ.Ｔｈｅｔｒａｎｓｉｅｎｔｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｉｅｓｏｆｔｈｅｓａｍｐｌｅｗｅｒｅｍｅａｓｕｒｅｄａｔａｎａｎｎｅａｌｅｄｓｔａｔｅａｎｄｌｉｇｈｔ ｓｏａｋｅｄｓｔａｔｅｓ.Ｔｈｅｔｒａｎｓｉｅｎｔｄｅｃａｙｐｒｏｃｅｓｓｏｆｔｈｅｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙｃａｎｂｅｆｉｔｔｅｄｆａｉｒｌｙｗｅｌｌｂｙａｓｅｃｏｎｄ ｏｒｄｅｒｅｘｐｏｎｅｎｔｉａｌｄｅｃａｙｆｕｎｃｔｉｏｎ ,ｗｈｉｃｈｉｎｄｉｃａｔｅｓｔｈａｔｔｈｅｄｅｃａｙｐｒｏｃｅｓｓｉｓｒｅｌａｔｅｄｗｉｔｈｔｗｏｄｉｆｆｅｒｅｎｔｔｒａｐｓ.Ｉｔｉｓｎｏｔｅｗｏｒｔｈｙｔｈａｔｔｈｅｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙｏｆｔｈｅｆｉｌｍｉｎｃｒｅａｓｅｓａｆｔｅｒｌｉｇｈｔ ｓｏａｋｉｎｇ.ＴｈｉｓｍａｙｂｅｄｕｅｔｏｔｈｅｄｅａｃｔｉｖｉｔｙｏｆｔｈｅｂｏｒｏｎａｃｃｅｐｔｏｒＢ-4,ａｎｄｔｈｕｓｓｏｍｅｏｆｔｈｅｂｏｒｏｎａｔｏｍｓｃａｎｎｏｌｏｎｇｅｒａｃｔａｓａｃｃｅｐｔｏｒｓａｎｄｄｒｉｖｅｓＥＦｔｏｓｈｉｆｔｓｕｐｗａｒｄ .Ｃｏｎｓｅｑｕｅｎｔｌｙ,ｔｈｅｎｕｍｂｅｒｏｆｅｆｆｅｃｔｉｖｅｒｅｃｏｍｂｉｎａｔｉｏｎｃｅｎｔｅｒｓｍａｙｂｅｒｅｄｕｃｅｄａｎｄｓｏｔｈｅｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙｉｎｃｒｅａｓｅｓ.


Acta Physica Sinica. 2002 51(1): 111-114. Published 2005-04-11 ]]>

Ｔｒａｎｓｉｅｎｔｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙａｎｄｉｔｓｌｉｇｈｔ ｉｎｄｕｃｅｄｃｈａｎｇｅｗｅｒｅｉｎｖｅｓｔｉｇａｔｅｄｂｙｕｓｉｎｇａＭｏｄｅｌ440 0ｂｏｘｃａｒａｖｅｒａｇｅｒａｎｄｓｉｇｎａｌｐｒｏｃｅｓｓｏｒｆｏｒｌｉｇｈｔｌｙｂｏｒｏｎ ｄｏｐｅｄａ Ｓｉ∶Ｈｆｉｌｍｓ.Ｔｈｅｔｒａｎｓｉｅｎｔｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｉｅｓｏｆｔｈｅｓａｍｐｌｅｗｅｒｅｍｅａｓｕｒｅｄａｔａｎａｎｎｅａｌｅｄｓｔａｔｅａｎｄｌｉｇｈｔ ｓｏａｋｅｄｓｔａｔｅｓ.Ｔｈｅｔｒａｎｓｉｅｎｔｄｅｃａｙｐｒｏｃｅｓｓｏｆｔｈｅｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙｃａｎｂｅｆｉｔｔｅｄｆａｉｒｌｙｗｅｌｌｂｙａｓｅｃｏｎｄ ｏｒｄｅｒｅｘｐｏｎｅｎｔｉａｌｄｅｃａｙｆｕｎｃｔｉｏｎ ,ｗｈｉｃｈｉｎｄｉｃａｔｅｓｔｈａｔｔｈｅｄｅｃａｙｐｒｏｃｅｓｓｉｓｒｅｌａｔｅｄｗｉｔｈｔｗｏｄｉｆｆｅｒｅｎｔｔｒａｐｓ.Ｉｔｉｓｎｏｔｅｗｏｒｔｈｙｔｈａｔｔｈｅｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙｏｆｔｈｅｆｉｌｍｉｎｃｒｅａｓｅｓａｆｔｅｒｌｉｇｈｔ ｓｏａｋｉｎｇ.ＴｈｉｓｍａｙｂｅｄｕｅｔｏｔｈｅｄｅａｃｔｉｖｉｔｙｏｆｔｈｅｂｏｒｏｎａｃｃｅｐｔｏｒＢ-4,ａｎｄｔｈｕｓｓｏｍｅｏｆｔｈｅｂｏｒｏｎａｔｏｍｓｃａｎｎｏｌｏｎｇｅｒａｃｔａｓａｃｃｅｐｔｏｒｓａｎｄｄｒｉｖｅｓＥＦｔｏｓｈｉｆｔｓｕｐｗａｒｄ .Ｃｏｎｓｅｑｕｅｎｔｌｙ,ｔｈｅｎｕｍｂｅｒｏｆｅｆｆｅｃｔｉｖｅｒｅｃｏｍｂｉｎａｔｉｏｎｃｅｎｔｅｒｓｍａｙｂｅｒｅｄｕｃｅｄａｎｄｓｏｔｈｅｐｈｏｔｏｃｏｎｄｕｃｔｉｖｉｔｙｉｎｃｒｅａｓｅｓ.


Acta Physica Sinica. 2002 51(1): 111-114. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 111-114. article doi:10.7498/aps.51.111 10.7498/aps.51.111 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.111 111-114 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.115

Ｉｒｏｎ ｓｉｌｉｃｉｄｅｆｉｌｍｓｈａｖｅｂｅｅｎｓｙｎｔｈｅｓｉｚｅｄｂｙｍｅｔａｌｖａｐｏｒｖａｃｕｕｍａｒｃ (ＭＥＶＶＡ)ｉｏｎｉｍｐｌａｎｔａｔｉｏｎｏｆｉｒｏｎｉｎｔｏ (1 1 1 )ａｎｄ(1 0 0 )ｏｒｉｅｎｔｅｄｓｉｌｉｃｏｎｗａｆｅｒｓ.Ｔｈｅｓｔｒｕｃｔｕｒｅｅｖｏｌｕｔｉｏｎｗａｓｃｈａｒａｃｔｅｒｉｚｅｄｕｓｉｎｇｔｒａｎｓｍｉｓｓｉｏｎｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｙ (ＴＥＭ)ａｎｄｈｉｇｈｒｅｓｏｌｕｔｉｏｎｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｙ (ＨＲＥＭ) .ＴｈｅβFeSi2ｆｉｌｍｓａｎｄｂｕｒｉｅｄｌａｙｅｒｓｗｉｔｈｄｉｆｆｅｒｅｎｔｄｅｐｔｈａｎｄｔｈｉｃｋｎｅｓｓｗｅｒｅｏｂｔａｉｎｅｄｂｙａｄｊｕｓｔｉｎｇｔｈｅｉｍｐｌａｎｔａｔｉｏｎｅｎｅｒｇｙａｎｄｄｏｓｅ .Ｔｈｅｆｏｒｍａｔｉｏｎｏｆα,β,γａｎｄＣｓＣｌ ＦｅＳｉ2 ｐｈａｓｅｓｈａｖｅｂｅｅｎｏｂｓｅｒｖｅｄ .ＴｈｅｐｈａｓｅｔｒａｎｓｉｔｉｏｎｏｒｄｅｒｉｓγFeSi2→βFeSi2→αFeSi2,CsClFeSi2→βFeSi2→αFeSi2 or βFeSi2→αFeSi2.Ａｎａｍｏｒｐｈｏｕｓｌａｙｅｒｗａｓｆｏｒｍｅｄａｔ60ｋＶａｎｄ 4× 1 0 1 7ｉｏｎｓ ｃｍ2 ,ｔｈｅｐｈａｓｅｔｒａｎｓｉｔｉｏｎｏｒｄｅｒｉｓａｍｏｒｐｈｏｕｓ→β ＦｅＳｉ2 →α ＦｅＳｉ2 .Ｔｈｅｍｏｒｐｈｏｌｏｇｙａｎｄｐｏｓｉｔｉｏｎｏｆｔｈｅｓｉｌｉｃｉｄｅｆｉｌｍｓｃｈａｎｇｅｗｉｔｈｔｈｅａｎｎｅａｌｉｎｇｔｅｍｐｅｒａｔｕｒｅ.Ｔｈｅｓｉｌｉｃｉｄｅｇｒａｉｎｓｇｒｏｗｗｉｔｈｉｎｃｒｅａｓｉｎｇａｎｎｅａｌｉｎｇｔｅｍｐｅｒａｔｕｒｅｗｉｔｈｆｕｒｔｈｅｒｉｎｃｒｅａｓｅｏｆｔｅｍｐｅｒａｔｕｒｅ ,ｔｈｅｃｏｎｔｉｎｕｏｕｓｓｉｌｉｃｉｄｅｌａｙｅｒｓｓｈｒｉｎｋｉｎｔｏｉｓｏｌａｔｅｄｉｓｌａｎｄｓａｎｄｔｈｅｉｎｔｅｒｆａｃｅβ ＦｅＳｉ2 Ｓｉｂｅ ｃｏｍｅｓｒｏｕｇｈｅｒ.Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｃｏｍｐｌｉｃａｔｅｄｏｒｉｅｎｔａｔｉｏｎｒｅｌａｔｉｏｎｓｈｉｐｓｅｘｉｓｔｉｎｇｂｅｔｗｅｅｎβ ＦｅＳｉ2 ａｎｄＳｉｗｅｒｅａｌｓｏｉｎｖｅｓｔｉｇａｔｅｄ


Acta Physica Sinica. 2002 51(1): 115-124. Published 2005-04-11 ]]>

Ｉｒｏｎ ｓｉｌｉｃｉｄｅｆｉｌｍｓｈａｖｅｂｅｅｎｓｙｎｔｈｅｓｉｚｅｄｂｙｍｅｔａｌｖａｐｏｒｖａｃｕｕｍａｒｃ (ＭＥＶＶＡ)ｉｏｎｉｍｐｌａｎｔａｔｉｏｎｏｆｉｒｏｎｉｎｔｏ (1 1 1 )ａｎｄ(1 0 0 )ｏｒｉｅｎｔｅｄｓｉｌｉｃｏｎｗａｆｅｒｓ.Ｔｈｅｓｔｒｕｃｔｕｒｅｅｖｏｌｕｔｉｏｎｗａｓｃｈａｒａｃｔｅｒｉｚｅｄｕｓｉｎｇｔｒａｎｓｍｉｓｓｉｏｎｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｙ (ＴＥＭ)ａｎｄｈｉｇｈｒｅｓｏｌｕｔｉｏｎｅｌｅｃｔｒｏｎｍｉｃｒｏｓｃｏｐｙ (ＨＲＥＭ) .ＴｈｅβFeSi2ｆｉｌｍｓａｎｄｂｕｒｉｅｄｌａｙｅｒｓｗｉｔｈｄｉｆｆｅｒｅｎｔｄｅｐｔｈａｎｄｔｈｉｃｋｎｅｓｓｗｅｒｅｏｂｔａｉｎｅｄｂｙａｄｊｕｓｔｉｎｇｔｈｅｉｍｐｌａｎｔａｔｉｏｎｅｎｅｒｇｙａｎｄｄｏｓｅ .Ｔｈｅｆｏｒｍａｔｉｏｎｏｆα,β,γａｎｄＣｓＣｌ ＦｅＳｉ2 ｐｈａｓｅｓｈａｖｅｂｅｅｎｏｂｓｅｒｖｅｄ .ＴｈｅｐｈａｓｅｔｒａｎｓｉｔｉｏｎｏｒｄｅｒｉｓγFeSi2→βFeSi2→αFeSi2,CsClFeSi2→βFeSi2→αFeSi2 or βFeSi2→αFeSi2.Ａｎａｍｏｒｐｈｏｕｓｌａｙｅｒｗａｓｆｏｒｍｅｄａｔ60ｋＶａｎｄ 4× 1 0 1 7ｉｏｎｓ ｃｍ2 ,ｔｈｅｐｈａｓｅｔｒａｎｓｉｔｉｏｎｏｒｄｅｒｉｓａｍｏｒｐｈｏｕｓ→β ＦｅＳｉ2 →α ＦｅＳｉ2 .Ｔｈｅｍｏｒｐｈｏｌｏｇｙａｎｄｐｏｓｉｔｉｏｎｏｆｔｈｅｓｉｌｉｃｉｄｅｆｉｌｍｓｃｈａｎｇｅｗｉｔｈｔｈｅａｎｎｅａｌｉｎｇｔｅｍｐｅｒａｔｕｒｅ.Ｔｈｅｓｉｌｉｃｉｄｅｇｒａｉｎｓｇｒｏｗｗｉｔｈｉｎｃｒｅａｓｉｎｇａｎｎｅａｌｉｎｇｔｅｍｐｅｒａｔｕｒｅｗｉｔｈｆｕｒｔｈｅｒｉｎｃｒｅａｓｅｏｆｔｅｍｐｅｒａｔｕｒｅ ,ｔｈｅｃｏｎｔｉｎｕｏｕｓｓｉｌｉｃｉｄｅｌａｙｅｒｓｓｈｒｉｎｋｉｎｔｏｉｓｏｌａｔｅｄｉｓｌａｎｄｓａｎｄｔｈｅｉｎｔｅｒｆａｃｅβ ＦｅＳｉ2 Ｓｉｂｅ ｃｏｍｅｓｒｏｕｇｈｅｒ.Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｃｏｍｐｌｉｃａｔｅｄｏｒｉｅｎｔａｔｉｏｎｒｅｌａｔｉｏｎｓｈｉｐｓｅｘｉｓｔｉｎｇｂｅｔｗｅｅｎβ ＦｅＳｉ2 ａｎｄＳｉｗｅｒｅａｌｓｏｉｎｖｅｓｔｉｇａｔｅｄ


Acta Physica Sinica. 2002 51(1): 115-124. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 115-124. article doi:10.7498/aps.51.115 10.7498/aps.51.115 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.115 115-124 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.125

ＴｈｉｓｐａｐｅｒｐｒｅｓｅｎｔｓａｓｔｕｄｙｏｎｅｌｅｃｔｒｏｎｉｃｓｔｒｕｃｔｕｒｅｓｏｆｄｅｆｅｃｔｓａｓｓｏｃｉａｔｅｄｗｉｔｈｏｘｙｇｅｎｖａｃａｎｃｙＶＯａｎｄｌｅａｄｖａｃａｎｃｙＶＰｂｉｎｌｅａｄｔｕｎｇｓｔａｔｅｃｒｙｓｔａｌｓ (ＰｂＷＯ4) ,ｂｙｔｈｅｒｅｌａｔｉｖｉｓｔｉｃｓｅｌｆ ｃｏｎｓｉｓｔｅｎｔｄｉｓｃｒｅｔｅｖａｒｉａｔｉｏｎａｌｅｍｂｅｄｄｅｄｃｌｕｓｔｅｒｍｅｔｈｏｄ .Ｆｕｒｔｈｅｒｍｏｒｅ,ｔｈｅｅｘｃｉｔａｔｉｏｎｅｎｅｒｇｙｉｓａｌｓｏｃａｌｃｕｌａｔｅｄ.ＷｅｆｏｕｎｄｔｈａｔＷＯ3 +ＶＯｃｏｕｌｄｂｅｔｈｅａｂｓｏｒｐｔｉｏｎｃｅｎｔｅｒａｔ3 50ｎｍａｎｄ 42 0ｎｍ ,ａｎｄｔｈｅｅｘｉｓｔｅｎｃｅｏｆＶＰｂｃａｎｄｉｍｉｎｉｓｈｔｈｅｂａｎｄｇａｐｏｆＷＯ42 -.


Acta Physica Sinica. 2002 51(1): 125-128. Published 2005-04-11 ]]>

ＴｈｉｓｐａｐｅｒｐｒｅｓｅｎｔｓａｓｔｕｄｙｏｎｅｌｅｃｔｒｏｎｉｃｓｔｒｕｃｔｕｒｅｓｏｆｄｅｆｅｃｔｓａｓｓｏｃｉａｔｅｄｗｉｔｈｏｘｙｇｅｎｖａｃａｎｃｙＶＯａｎｄｌｅａｄｖａｃａｎｃｙＶＰｂｉｎｌｅａｄｔｕｎｇｓｔａｔｅｃｒｙｓｔａｌｓ (ＰｂＷＯ4) ,ｂｙｔｈｅｒｅｌａｔｉｖｉｓｔｉｃｓｅｌｆ ｃｏｎｓｉｓｔｅｎｔｄｉｓｃｒｅｔｅｖａｒｉａｔｉｏｎａｌｅｍｂｅｄｄｅｄｃｌｕｓｔｅｒｍｅｔｈｏｄ .Ｆｕｒｔｈｅｒｍｏｒｅ,ｔｈｅｅｘｃｉｔａｔｉｏｎｅｎｅｒｇｙｉｓａｌｓｏｃａｌｃｕｌａｔｅｄ.ＷｅｆｏｕｎｄｔｈａｔＷＯ3 +ＶＯｃｏｕｌｄｂｅｔｈｅａｂｓｏｒｐｔｉｏｎｃｅｎｔｅｒａｔ3 50ｎｍａｎｄ 42 0ｎｍ ,ａｎｄｔｈｅｅｘｉｓｔｅｎｃｅｏｆＶＰｂｃａｎｄｉｍｉｎｉｓｈｔｈｅｂａｎｄｇａｐｏｆＷＯ42 -.


Acta Physica Sinica. 2002 51(1): 125-128. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 125-128. article doi:10.7498/aps.51.125 10.7498/aps.51.125 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.125 125-128 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.129

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｓｏｆｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｒｅｓｉｓｔａｎｃｅｂｅｔｗｅｅｎ 0.1Ｋｔｏ 2 50Ｋａｎｄｓｐｅｃｉｆｉｃｈｅａｔｂｅｔｗｅｅｎ5Ｋｔｏ 70ＫｏｆｈｅａｖｙｆｅｒｍｉｏｎｃｏｍｐｏｕｎｄｓＣｅＣｕ6 ｘＮｉｘ(ｘ =0.0 ,0.0 5,0.1 ,0.15,0.2 )ａｒｅｒｅｐｏｒｔｅｄ .ＴｈｅｄｏｐｉｎｇｅｆｆｅｃｔｏｆｔｈｅＮｉｃｏｎｔｅｎｔｏｎｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｐｒｏｐｅｒｔｉｅｓｏｆＣｅＣｕ6 ｉｓｓｔｕｄｉｅｄ .Ｔｈｅｔｅｍｐｅｒａｔｕｒｅｓｏｆｒｅｓｉｓｔａｎｃｅｍａｘｉｍｕａｓｏｆｔｈｅｓａｍｐｌｅｓｒｅｄｕｃｅｄｒａｍａｔｉｃａｌｌｙｗｉｔｈｔｈｅｉｎｃｒｅａｓｅｏｆｔｈｅｄｏｐｉｎｇｃｏｎｔｅｎｔｘ.ＴｈｉｓｉｎｄｉｃａｔｅｓｔｈｅｅｎｈａｎｃｅｍｅｎｔｏｆｍａｇｎｅｔｉｃｍｏｍｅｎｔｏｆｍｉｎｏｒＣｅｉｏｎｓｔｈａｔａｒｅｎｅｉｇｈｂｏｒｉｎｇＮｉａｔｏｍａｎｄｔｈｅｄｅｃｒｅａｓｅｏｆｔｈｅｃｏｈｅｒｅｎｔｓｃａｔｔｅｒｉｎｇｂｅｔｗｅｅｎｔｈｅｗｈｏｌｅＣｅｉｏｎｌａｔｔｉｃｅａｎｄｔｈｅｃｏｎｄｕｃｔｉｏｎｅｌｅｃｔｒｏｎｓ.Ｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｅｌｅｃｔｒｏｎｉｃｓｐｅｃｉｆｉｃｈｅａｔｃｏｅｆｆｉｃｉｅｎｔγ(ＣＥ Ｔ ,ｗｈｅｒｅＣＥｉｓｔｈｅｅｌｅｃｔｒｏｎｉｃｓｐｅｃｉｆｉｃｈｅａｔ)ｉｓｎｅａｒｌｙａｃｏｎｓｔａｎｔａｔｌｏｗｔｅｍｐｅｒａｔｕｒｅｓ,ｂｕｔｉｔａｐｐａｒｅｎｔｌｙｉｎｃｒｅａｓｅｓｂｅｌｏｗ 8Ｋｄｕｅｔｏｔｈｅｉｎｃｒｅａｓｅｏｆｉｔｓｅｆｆｅｃｔｉｖｅｍａｓｓ.Ｈｏｗｅｖｅｒ,ｔｈｅｔｅｍ ｐｅｒａｔｕｒｅａｔｗｈｉｃｈγｂｅｇｉｎｓｔｏｉｎｃｒｅａｓｅｉｓｎｏｔｓｅｎｓｉｔｉｖｅｔｏｔｈｅｃｏｎｔｅｎｔｏｆＮｉ,ｉｎｄｉｃａｔｉｎｇｔｈａｔｔｈｅｓｔａｔｕｓｏｆｍｏｓｔｃｅｒｉｕｍｉｏｎｓａｒｅｎｏｔａｆｆｅｃｔｅｄ.


Acta Physica Sinica. 2002 51(1): 129-133. Published 2005-04-11 ]]>

Ｉｎｔｈｉｓｐａｐｅｒ,ｔｈｅｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｓｏｆｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｒｅｓｉｓｔａｎｃｅｂｅｔｗｅｅｎ 0.1Ｋｔｏ 2 50Ｋａｎｄｓｐｅｃｉｆｉｃｈｅａｔｂｅｔｗｅｅｎ5Ｋｔｏ 70ＫｏｆｈｅａｖｙｆｅｒｍｉｏｎｃｏｍｐｏｕｎｄｓＣｅＣｕ6 ｘＮｉｘ(ｘ =0.0 ,0.0 5,0.1 ,0.15,0.2 )ａｒｅｒｅｐｏｒｔｅｄ .ＴｈｅｄｏｐｉｎｇｅｆｆｅｃｔｏｆｔｈｅＮｉｃｏｎｔｅｎｔｏｎｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｐｒｏｐｅｒｔｉｅｓｏｆＣｅＣｕ6 ｉｓｓｔｕｄｉｅｄ .Ｔｈｅｔｅｍｐｅｒａｔｕｒｅｓｏｆｒｅｓｉｓｔａｎｃｅｍａｘｉｍｕａｓｏｆｔｈｅｓａｍｐｌｅｓｒｅｄｕｃｅｄｒａｍａｔｉｃａｌｌｙｗｉｔｈｔｈｅｉｎｃｒｅａｓｅｏｆｔｈｅｄｏｐｉｎｇｃｏｎｔｅｎｔｘ.ＴｈｉｓｉｎｄｉｃａｔｅｓｔｈｅｅｎｈａｎｃｅｍｅｎｔｏｆｍａｇｎｅｔｉｃｍｏｍｅｎｔｏｆｍｉｎｏｒＣｅｉｏｎｓｔｈａｔａｒｅｎｅｉｇｈｂｏｒｉｎｇＮｉａｔｏｍａｎｄｔｈｅｄｅｃｒｅａｓｅｏｆｔｈｅｃｏｈｅｒｅｎｔｓｃａｔｔｅｒｉｎｇｂｅｔｗｅｅｎｔｈｅｗｈｏｌｅＣｅｉｏｎｌａｔｔｉｃｅａｎｄｔｈｅｃｏｎｄｕｃｔｉｏｎｅｌｅｃｔｒｏｎｓ.Ｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｅｌｅｃｔｒｏｎｉｃｓｐｅｃｉｆｉｃｈｅａｔｃｏｅｆｆｉｃｉｅｎｔγ(ＣＥ Ｔ ,ｗｈｅｒｅＣＥｉｓｔｈｅｅｌｅｃｔｒｏｎｉｃｓｐｅｃｉｆｉｃｈｅａｔ)ｉｓｎｅａｒｌｙａｃｏｎｓｔａｎｔａｔｌｏｗｔｅｍｐｅｒａｔｕｒｅｓ,ｂｕｔｉｔａｐｐａｒｅｎｔｌｙｉｎｃｒｅａｓｅｓｂｅｌｏｗ 8Ｋｄｕｅｔｏｔｈｅｉｎｃｒｅａｓｅｏｆｉｔｓｅｆｆｅｃｔｉｖｅｍａｓｓ.Ｈｏｗｅｖｅｒ,ｔｈｅｔｅｍ ｐｅｒａｔｕｒｅａｔｗｈｉｃｈγｂｅｇｉｎｓｔｏｉｎｃｒｅａｓｅｉｓｎｏｔｓｅｎｓｉｔｉｖｅｔｏｔｈｅｃｏｎｔｅｎｔｏｆＮｉ,ｉｎｄｉｃａｔｉｎｇｔｈａｔｔｈｅｓｔａｔｕｓｏｆｍｏｓｔｃｅｒｉｕｍｉｏｎｓａｒｅｎｏｔａｆｆｅｃｔｅｄ.


Acta Physica Sinica. 2002 51(1): 129-133. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 129-133. article doi:10.7498/aps.51.129 10.7498/aps.51.129 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.129 129-133 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.134

Ｈｏｗｔｏｅｘｃｉｔｅｔｈｅｂｉｅｘｃｔｉｏｎｓｉｎａｐｏｌｙｍｅｒｉｓａｎｅｓｓｅｎｔｉａｌｓｕｂｊｅｃｔ,ｓｉｎｃｅｔｈｅｂｉｅｘｃｉｔｏｎｐｏｓｓｅｓｓｅｓａｎｅｆｆｅｃｔｏｆｐｈｏｔｏ ｉｎｄｕｃｅｄｐｏｌａｒｉｚａｔｉｏｎｒｅｖｅｒｓｉｏｎ.Ｔｈｉｓｐａｐｅｒｐｒｏｐｏｓｅｓａｎｅｗｃｈａｎｎｅｌｔｏｐｒｏｄｕｃｅｔｈｅｂｉｅｘｃｉｔｏｎｔｈｒｏｕｇｈｔｗｏ ｅｌｅｃｔｒｏｎｅｘｃｉｔａｔｉｏｎ.Ｔｈｅｒｅｌａｘａｔｉｏｎｐｒｏｃｅｓｓｅｓｏｆｂｏｔｈｌａｔｔｉｃｅｄｉｓｔｏｒｔｉｏｎａｎｄｅｌｅｃｔｒｏｎｉｃｓｔａｔｅｓａｒｅｓｉｍｕｌａｔｅｄｂｙｓｔｕｄｙｉｎｇｉｔｓｄｙｎａｍｉｃｓ,ａｎｄｔｈｅｒｅｌａｘａｔｉｏｎｔｉｍｅｏｆｂｉｅｘｃｉｔｏｎｆｏｒｍａｔｉｏｎａｎｄｐｏｌａｒｉｚａｔｉｏｎｒｅｖｅｒｓｉｏｎｉｓｄｅｔｅｒｍｉｎｅｄ .


Acta Physica Sinica. 2002 51(1): 134-137. Published 2005-04-11 ]]>

Ｈｏｗｔｏｅｘｃｉｔｅｔｈｅｂｉｅｘｃｔｉｏｎｓｉｎａｐｏｌｙｍｅｒｉｓａｎｅｓｓｅｎｔｉａｌｓｕｂｊｅｃｔ,ｓｉｎｃｅｔｈｅｂｉｅｘｃｉｔｏｎｐｏｓｓｅｓｓｅｓａｎｅｆｆｅｃｔｏｆｐｈｏｔｏ ｉｎｄｕｃｅｄｐｏｌａｒｉｚａｔｉｏｎｒｅｖｅｒｓｉｏｎ.Ｔｈｉｓｐａｐｅｒｐｒｏｐｏｓｅｓａｎｅｗｃｈａｎｎｅｌｔｏｐｒｏｄｕｃｅｔｈｅｂｉｅｘｃｉｔｏｎｔｈｒｏｕｇｈｔｗｏ ｅｌｅｃｔｒｏｎｅｘｃｉｔａｔｉｏｎ.Ｔｈｅｒｅｌａｘａｔｉｏｎｐｒｏｃｅｓｓｅｓｏｆｂｏｔｈｌａｔｔｉｃｅｄｉｓｔｏｒｔｉｏｎａｎｄｅｌｅｃｔｒｏｎｉｃｓｔａｔｅｓａｒｅｓｉｍｕｌａｔｅｄｂｙｓｔｕｄｙｉｎｇｉｔｓｄｙｎａｍｉｃｓ,ａｎｄｔｈｅｒｅｌａｘａｔｉｏｎｔｉｍｅｏｆｂｉｅｘｃｉｔｏｎｆｏｒｍａｔｉｏｎａｎｄｐｏｌａｒｉｚａｔｉｏｎｒｅｖｅｒｓｉｏｎｉｓｄｅｔｅｒｍｉｎｅｄ .


Acta Physica Sinica. 2002 51(1): 134-137. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 134-137. article doi:10.7498/aps.51.134 10.7498/aps.51.134 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.134 134-137 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.138

ＶｏｌｔａｇｅｔｒａｎｓｉｅｎｔｓｄｕｅｔｏｔｈｅｔｈｅｒｍａｌｅｌｅｃｔｒｏｎｃａｐｔｕｒｅａｎｄｅｍｉｓｓｉｏｎｏｆＤＸｃｅｎｔｅｒｓｉｎｎ ｔｙｐｅＳｎ ｄｏｐｅｄＡｌ0 . 2 6 Ｇａ0 .74ＡｓｗｅｒｅｍｅａｓｕｒｅｄｂｙｔｈｅｃｏｎｓｔａｎｔｃａｐａｃｉｔａｎｃｅｔｅｃｈｎｉｑｕｅａｎｄｔｒａｎｓｆｏｒｍｅｄｂｙＬａｐｌａｃｅｄｅｆｅｃｔｓｐｅｃｔｒｏｓｃｏｐｙ (ＬＤＳ) .Ｂｙａｎａｌｙｚｉｎｇｔｈｅｖａｒｉａｔｉｏｎｓｏｆｄｉｓｃｒｅｔｅｅｍｉｓｓｉｏｎｒａｔｅｓｗｉｔｈｄｉｆｆｅｒｅｎｔｃａｐｔｕｒｅｐｅｒｉｏｄｓ,ｃｏｒｒｅｓｐｏｎｄｉｎｇｒｅｌａｔｉｏｎｓｂｅｔｗｅｅｎｄｉｓｃｒｅｔｅｃａｐｔｕｒｅａｎｄｅｍｉｓｓｉｏｎｒａｔｅｓａｎｄｃａｐｔｕｒｅｃｏｅｆｆｉｃｉｅｎｔｓｗｅｒｅｄｅｔｅｒｍｉｎｅｄ .ＴｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｓｏｆｅｌｅｃｔｒｏｎｃａｐｔｕｒｅｂａｒｒｉｅｒｓｏｆｔｈｅＳｎ ｒｅｌａｔｅｄＤＸｃｅｎｔｅｒｓｗｅｒｅｏｂｔａｉｎｅｄｂｙｌｉｎｅａｒｆｉｔｔｉｎｇｔｈｅｄａｔａｏｆｔｅｍｐｅｒａｔｕｒｅ ｄｅｐｅｎｄｅｎｃｅｓｏｆｔｈｅｃａｐｔｕｒｅｃｏｅｆｆｉｃｉｅｎｔｓ.ＴｈｅｒｅｓｕｌｔｓｃａｌｃｕａｔｅｄｂｙｕｓｉｎｇｔｈｅｆｉｒｓｔｐｒｉｎｃｉｐｌｅｐｓｅｕｄｏｐｏｔｅｎｔｉａｌｍｅｔｈｏｄｓｈｏｗｔｈａｔｔｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｓｏｆｔｈｅｃａｐｔｕｒｅｂａｒｒｉｅｒｓｍａｉｎｌｙｃｏｎｔｒｉｂｕｔｅｔｏＡｌ ＧａａｔｄｉｆｆｅｒｅｎｔｌｏｃａｌｃｏｎｆｉｇｕｒａｔｉｏｎｓｎｅａｒＳｎａｔｏｍｓｄｕｅｔｏｔｈｅａｌｌｏｙｒａｎｄｏｍｅｆｆｅｃｔ.


Acta Physica Sinica. 2002 51(1): 138-142. Published 2005-04-11 ]]>

ＶｏｌｔａｇｅｔｒａｎｓｉｅｎｔｓｄｕｅｔｏｔｈｅｔｈｅｒｍａｌｅｌｅｃｔｒｏｎｃａｐｔｕｒｅａｎｄｅｍｉｓｓｉｏｎｏｆＤＸｃｅｎｔｅｒｓｉｎｎ ｔｙｐｅＳｎ ｄｏｐｅｄＡｌ0 . 2 6 Ｇａ0 .74ＡｓｗｅｒｅｍｅａｓｕｒｅｄｂｙｔｈｅｃｏｎｓｔａｎｔｃａｐａｃｉｔａｎｃｅｔｅｃｈｎｉｑｕｅａｎｄｔｒａｎｓｆｏｒｍｅｄｂｙＬａｐｌａｃｅｄｅｆｅｃｔｓｐｅｃｔｒｏｓｃｏｐｙ (ＬＤＳ) .Ｂｙａｎａｌｙｚｉｎｇｔｈｅｖａｒｉａｔｉｏｎｓｏｆｄｉｓｃｒｅｔｅｅｍｉｓｓｉｏｎｒａｔｅｓｗｉｔｈｄｉｆｆｅｒｅｎｔｃａｐｔｕｒｅｐｅｒｉｏｄｓ,ｃｏｒｒｅｓｐｏｎｄｉｎｇｒｅｌａｔｉｏｎｓｂｅｔｗｅｅｎｄｉｓｃｒｅｔｅｃａｐｔｕｒｅａｎｄｅｍｉｓｓｉｏｎｒａｔｅｓａｎｄｃａｐｔｕｒｅｃｏｅｆｆｉｃｉｅｎｔｓｗｅｒｅｄｅｔｅｒｍｉｎｅｄ .ＴｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｓｏｆｅｌｅｃｔｒｏｎｃａｐｔｕｒｅｂａｒｒｉｅｒｓｏｆｔｈｅＳｎ ｒｅｌａｔｅｄＤＸｃｅｎｔｅｒｓｗｅｒｅｏｂｔａｉｎｅｄｂｙｌｉｎｅａｒｆｉｔｔｉｎｇｔｈｅｄａｔａｏｆｔｅｍｐｅｒａｔｕｒｅ ｄｅｐｅｎｄｅｎｃｅｓｏｆｔｈｅｃａｐｔｕｒｅｃｏｅｆｆｉｃｉｅｎｔｓ.ＴｈｅｒｅｓｕｌｔｓｃａｌｃｕａｔｅｄｂｙｕｓｉｎｇｔｈｅｆｉｒｓｔｐｒｉｎｃｉｐｌｅｐｓｅｕｄｏｐｏｔｅｎｔｉａｌｍｅｔｈｏｄｓｈｏｗｔｈａｔｔｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｓｏｆｔｈｅｃａｐｔｕｒｅｂａｒｒｉｅｒｓｍａｉｎｌｙｃｏｎｔｒｉｂｕｔｅｔｏＡｌ ＧａａｔｄｉｆｆｅｒｅｎｔｌｏｃａｌｃｏｎｆｉｇｕｒａｔｉｏｎｓｎｅａｒＳｎａｔｏｍｓｄｕｅｔｏｔｈｅａｌｌｏｙｒａｎｄｏｍｅｆｆｅｃｔ.


Acta Physica Sinica. 2002 51(1): 138-142. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 138-142. article doi:10.7498/aps.51.138 10.7498/aps.51.138 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.138 138-142 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.143

Ａｃｏｎｄｕｃｔａｎｃｅｍｏｄｅｌｏｆｅｌｅｃｔｒｏｎｉｃｔｕｎｎｅｌｉｎｇｔｒａｎｓｆｅｒｉｓｓｅｔｕｐ,ａｎｄａｎｅｗＤ .Ｃｃｏｎｄｕｃｔａｎｃｅｆｏｒｍｕｌａｉｎｏｎｅ ｄｉｍｅｎｓｉｏｎａｌｄｉｓｏｒｄｅｒｅｄｓｙｓｔｅｍｉｓｄｅｒｉｖｅｄ .ＢｙｃａｌｃｕｌａｔｉｎｇｔｈｅＤ .Ｃｃｏｎｄｕｃｔｉｖｉｔｙ,ｔｈｅｒｅｌａｔｉｏｎｓｈｉｐａｍｏｎｇｔｈｅｅｌｅｃｔｒｉｃｆｉｅｌｄ、ｔｅｍｐｅｒａｔｕｒｅａｎｄｃｏｎｄｕｃｔｉｖｉｔｙｉｓａｎａｌｙｚｅｄ ,ａｎｄｔｈｅｅｆｆｅｃｔｏｆｄｉｓｏｒｄｅｒｅｄｄｅｇｒｅｅｏｎｔｈｅＤ .Ｃｃｏｎｄｕｃｔａｎｃｅｉｓｄｉｓｃｕｓｓｅｄ .Ｔｈｅｒｅｓｕｌｔｓｈｏｗｓｔｈａｔｔｈｅｃｏｎｄｕｃｔｉｖｉｔｙｏｆａｄｉｓｏｒｄｅｒｅｄｓｙｓｔｅｍｄｅｃｒｅａｓｅｓｗｉｔｈｔｈｅｉｎｃｒｅａｓｅｏｆｄｉｓｏｒｄｅｒｅｄｄｅｇｒｅｅ.Ｗｈｅｎｔｈｅｅｌｅｃｔｒｉｃｆｉｅｌｄｉｓｗｅａｋ ,ｉｔｓｃｏｎｄｕｃｔｉｖｉｔｙｉｓｈｉｇｈａｎｄｈａｓａｓｅｒｉｅｓｏｆｐｅａｋｖａｌｕｅｓ.Ｈｅｗｅｖｅｒ,ｗｈｅｎｔｈｅｅｌｅｃｔｒｉｃｆｉｅｌｄｉｓｓｔｒｏｎｇ,ｉｔｓｃｏｎｄｕｃｔｉｖｉｔｙｉｓｗｅａｋ.Ｉｎｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｒｅｇｉｏｎ,ｔｈｅｄｉｓｏｒｄｅｒｅｄｓｙｓｔｅｍｓｈｏｗｓａｃｈａｒａｃｔｅｒｉｓｔｉｃｏｆｎｅｇａｔｉｖｅｄｉｆｆｅｒｅｎｔｉａｌｄｅｐｅｎｄｅｎｃｅｏｆｒｅｓｉｓｔａｎｃｅａｎｄｔｅｍｐｅｒａｔｕｒｅ.Ｏｎｔｈｅｃｏｎｔｒａｒｙ,ｉｔｓｃｏｎｄｕｃｔｉｖｉｔｙｄｅｃｒｅａｓｅｓｗｉｔｈｔｈｅｒｉｓｅｏｆｔｅｍｐｅｒａｔｕｒｅｉｎｔｈｅｈｉｇｈ ｔｅｍｐｅｒａｔｕｒｅｒｅｇｉｏｎ.Ｔｈｉｓｒｅｓｕｌｔｉｓｉｎｇｏｏｄａｇｒｅｅｍｅｎｔｗｉｔｈｔｈｅｅｘｐｅｒｉｍｅｎｔｓ.


Acta Physica Sinica. 2002 51(1): 143-147. Published 2005-04-11 ]]>

Ａｃｏｎｄｕｃｔａｎｃｅｍｏｄｅｌｏｆｅｌｅｃｔｒｏｎｉｃｔｕｎｎｅｌｉｎｇｔｒａｎｓｆｅｒｉｓｓｅｔｕｐ,ａｎｄａｎｅｗＤ .Ｃｃｏｎｄｕｃｔａｎｃｅｆｏｒｍｕｌａｉｎｏｎｅ ｄｉｍｅｎｓｉｏｎａｌｄｉｓｏｒｄｅｒｅｄｓｙｓｔｅｍｉｓｄｅｒｉｖｅｄ .ＢｙｃａｌｃｕｌａｔｉｎｇｔｈｅＤ .Ｃｃｏｎｄｕｃｔｉｖｉｔｙ,ｔｈｅｒｅｌａｔｉｏｎｓｈｉｐａｍｏｎｇｔｈｅｅｌｅｃｔｒｉｃｆｉｅｌｄ、ｔｅｍｐｅｒａｔｕｒｅａｎｄｃｏｎｄｕｃｔｉｖｉｔｙｉｓａｎａｌｙｚｅｄ ,ａｎｄｔｈｅｅｆｆｅｃｔｏｆｄｉｓｏｒｄｅｒｅｄｄｅｇｒｅｅｏｎｔｈｅＤ .Ｃｃｏｎｄｕｃｔａｎｃｅｉｓｄｉｓｃｕｓｓｅｄ .Ｔｈｅｒｅｓｕｌｔｓｈｏｗｓｔｈａｔｔｈｅｃｏｎｄｕｃｔｉｖｉｔｙｏｆａｄｉｓｏｒｄｅｒｅｄｓｙｓｔｅｍｄｅｃｒｅａｓｅｓｗｉｔｈｔｈｅｉｎｃｒｅａｓｅｏｆｄｉｓｏｒｄｅｒｅｄｄｅｇｒｅｅ.Ｗｈｅｎｔｈｅｅｌｅｃｔｒｉｃｆｉｅｌｄｉｓｗｅａｋ ,ｉｔｓｃｏｎｄｕｃｔｉｖｉｔｙｉｓｈｉｇｈａｎｄｈａｓａｓｅｒｉｅｓｏｆｐｅａｋｖａｌｕｅｓ.Ｈｅｗｅｖｅｒ,ｗｈｅｎｔｈｅｅｌｅｃｔｒｉｃｆｉｅｌｄｉｓｓｔｒｏｎｇ,ｉｔｓｃｏｎｄｕｃｔｉｖｉｔｙｉｓｗｅａｋ.Ｉｎｔｈｅｌｏｗ ｔｅｍｐｅｒａｔｕｒｅｒｅｇｉｏｎ,ｔｈｅｄｉｓｏｒｄｅｒｅｄｓｙｓｔｅｍｓｈｏｗｓａｃｈａｒａｃｔｅｒｉｓｔｉｃｏｆｎｅｇａｔｉｖｅｄｉｆｆｅｒｅｎｔｉａｌｄｅｐｅｎｄｅｎｃｅｏｆｒｅｓｉｓｔａｎｃｅａｎｄｔｅｍｐｅｒａｔｕｒｅ.Ｏｎｔｈｅｃｏｎｔｒａｒｙ,ｉｔｓｃｏｎｄｕｃｔｉｖｉｔｙｄｅｃｒｅａｓｅｓｗｉｔｈｔｈｅｒｉｓｅｏｆｔｅｍｐｅｒａｔｕｒｅｉｎｔｈｅｈｉｇｈ ｔｅｍｐｅｒａｔｕｒｅｒｅｇｉｏｎ.Ｔｈｉｓｒｅｓｕｌｔｉｓｉｎｇｏｏｄａｇｒｅｅｍｅｎｔｗｉｔｈｔｈｅｅｘｐｅｒｉｍｅｎｔｓ.


Acta Physica Sinica. 2002 51(1): 143-147. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 143-147. article doi:10.7498/aps.51.143 10.7498/aps.51.143 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.143 143-147 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.148

Ａｌａｒｇｅ ｓｉｇｎａｌａｎａｌｙｔｉｃａｌｍｏｄｅｌｗｉｔｈｔｅｍｐｅｒａｔｕｒｅｃｏｎｓｉｄｅｒｅｄｆｏｒ4Ｈ ＳｉＣｒａｄｉｏｆｒｅｑｕｅｎｃｙｐｏｗｅｒＭＥＳＦＥＴＩ Ｖｃｈａｒａｃｔｅｒｉｓｔｉｃｓｉｓｐｒｏｐｏｓｅｄｂａｓｅｄｏｎｔｈｅｔｈｅｏｒｙｏｆｓａｔｕｒａｔｅｄｃａｒｒｉｅｒｖｅｌｏｃｉｔｙ,ｂｙｍｅａｎｓｏｆｗｈｉｃｈｔｈｅｓｅｌｆ ｈｅａｔｉｎｇｅｆｆｅｃｔｉｓｔａｋｅｎｉｎｔｏａｃｃｏｕｎｔｓｏａｓｔｏａｎａｌｙｚｅｔｈｅｔｅｍｐｅｒａｔｕｒｅｐｅｒｆｏｒｍａｎｃｅｏｆＳｉＣｐｏｗｅｒＭＥＳＦＥＴ .Ｔｈｅｈｅａｔｔｒａｎｓｐｏｒｔｂｅｔｗｅｅｎｔｈｅｃｈａｎｎｅｌａｎｄｔｈｅｓｕｂｓｔｒａｔｅｉｓｍｏｄｅｌｅｄｗｉｔｈｎｏｎ ｃｏｎｓｔａｎｔｔｅｍｐｅｒａｔｕｒｅＴ0 ａｔｔｈｅｂｏｔｔｏｍｏｆ4Ｈ ＳｉＣｓｕｂｓｔｒａｔｅｉｎｏｒｄｅｒｔｏｆｉｔｔｈｅｒｅａｌａｃｔｉｏｎｓｏｆｄｅｖｉｃｅｓ.Ａｇｏｏｄａｇｒｅｅ ｍｅｎｔｂｅｔｗｅｅｎｓｉｍｕｌａｔｉｏｎａｎｄｍｅａｓｕｒｅｍｅｎｔｉｓｏｂｔａｉｎｅｄ.


Acta Physica Sinica. 2002 51(1): 148-152. Published 2005-04-11 ]]>

Ａｌａｒｇｅ ｓｉｇｎａｌａｎａｌｙｔｉｃａｌｍｏｄｅｌｗｉｔｈｔｅｍｐｅｒａｔｕｒｅｃｏｎｓｉｄｅｒｅｄｆｏｒ4Ｈ ＳｉＣｒａｄｉｏｆｒｅｑｕｅｎｃｙｐｏｗｅｒＭＥＳＦＥＴＩ Ｖｃｈａｒａｃｔｅｒｉｓｔｉｃｓｉｓｐｒｏｐｏｓｅｄｂａｓｅｄｏｎｔｈｅｔｈｅｏｒｙｏｆｓａｔｕｒａｔｅｄｃａｒｒｉｅｒｖｅｌｏｃｉｔｙ,ｂｙｍｅａｎｓｏｆｗｈｉｃｈｔｈｅｓｅｌｆ ｈｅａｔｉｎｇｅｆｆｅｃｔｉｓｔａｋｅｎｉｎｔｏａｃｃｏｕｎｔｓｏａｓｔｏａｎａｌｙｚｅｔｈｅｔｅｍｐｅｒａｔｕｒｅｐｅｒｆｏｒｍａｎｃｅｏｆＳｉＣｐｏｗｅｒＭＥＳＦＥＴ .Ｔｈｅｈｅａｔｔｒａｎｓｐｏｒｔｂｅｔｗｅｅｎｔｈｅｃｈａｎｎｅｌａｎｄｔｈｅｓｕｂｓｔｒａｔｅｉｓｍｏｄｅｌｅｄｗｉｔｈｎｏｎ ｃｏｎｓｔａｎｔｔｅｍｐｅｒａｔｕｒｅＴ0 ａｔｔｈｅｂｏｔｔｏｍｏｆ4Ｈ ＳｉＣｓｕｂｓｔｒａｔｅｉｎｏｒｄｅｒｔｏｆｉｔｔｈｅｒｅａｌａｃｔｉｏｎｓｏｆｄｅｖｉｃｅｓ.Ａｇｏｏｄａｇｒｅｅ ｍｅｎｔｂｅｔｗｅｅｎｓｉｍｕｌａｔｉｏｎａｎｄｍｅａｓｕｒｅｍｅｎｔｉｓｏｂｔａｉｎｅｄ.


Acta Physica Sinica. 2002 51(1): 148-152. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 148-152. article doi:10.7498/aps.51.148 10.7498/aps.51.148 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.148 148-152 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.153

Ｗｅｈａｖｅｏｂｓｅｒｖｅｄｔｈａｔａｗｅａｋｌｉｇｈｔｂｅａｍｗｉｌｌｅｘｐｅｒｉｅｎｃｅａｄｅｆｏｃｕｓｉｎｇ ｃｏｎｔｒａｃｔｐｒｏｃｅｓｓｂｅｆｏｒｅｉｔｃｏｍｅｓｔｏｓｔｅａｄｙｓｔａｔｅｗｈｅｎｐａｓｓｉｎｇｔｈｒｏｕｇｈａＣｕ:ＫＮＳＢＮｃｒｙｓｔａｌｗｉｔｈａｔｒａｎｓｉｅｎｔｓｐａｔｉａｌｅｌｅｃｔｒｉｃｆｉｅｌｄ.Ｔｈｉｓｐｒｏｃｅｓｓｂｅｃａｍｅｆａｓｔｂｙｉｎｃｒｅａｓｉｎｇｉｎｔｅｎｓｉｔｙｏｆｔｈｅｌｉｇｈｔｂｅａｍ .Ｗｅｂｅｌｉｅｖｅｔｈａｔｔｈｅｄｅｆｏｃｕｓｉｎｇ ｃｏｎｔｒａｃｔｐｒｏｃｅｓｓｒｅｓｕｌｔｓｆｒｏｍｂｏｔｈｅｆｆｅｃｔｓｏｆｔｈｅｔｒａｎｓｉｅｎｔｅｌｅｃｔｒｉｃｆｉｅｌｄｉｎｔｈｅｃｒｙｓｔａｌｓａｎｄｔｈｅｐｈｏｔｏｖｏｌｔａｉｃａｎｄｒｅｆｏｃｕｓｉｎｇｆｉｅｌｄｓｇｅｎｅｒａｔｅｄｂｙｔｈｅｂｅａｍｉｔｓｅｌｆ.


Acta Physica Sinica. 2002 51(1): 153-158. Published 2005-04-11 ]]>

Ｗｅｈａｖｅｏｂｓｅｒｖｅｄｔｈａｔａｗｅａｋｌｉｇｈｔｂｅａｍｗｉｌｌｅｘｐｅｒｉｅｎｃｅａｄｅｆｏｃｕｓｉｎｇ ｃｏｎｔｒａｃｔｐｒｏｃｅｓｓｂｅｆｏｒｅｉｔｃｏｍｅｓｔｏｓｔｅａｄｙｓｔａｔｅｗｈｅｎｐａｓｓｉｎｇｔｈｒｏｕｇｈａＣｕ:ＫＮＳＢＮｃｒｙｓｔａｌｗｉｔｈａｔｒａｎｓｉｅｎｔｓｐａｔｉａｌｅｌｅｃｔｒｉｃｆｉｅｌｄ.Ｔｈｉｓｐｒｏｃｅｓｓｂｅｃａｍｅｆａｓｔｂｙｉｎｃｒｅａｓｉｎｇｉｎｔｅｎｓｉｔｙｏｆｔｈｅｌｉｇｈｔｂｅａｍ .Ｗｅｂｅｌｉｅｖｅｔｈａｔｔｈｅｄｅｆｏｃｕｓｉｎｇ ｃｏｎｔｒａｃｔｐｒｏｃｅｓｓｒｅｓｕｌｔｓｆｒｏｍｂｏｔｈｅｆｆｅｃｔｓｏｆｔｈｅｔｒａｎｓｉｅｎｔｅｌｅｃｔｒｉｃｆｉｅｌｄｉｎｔｈｅｃｒｙｓｔａｌｓａｎｄｔｈｅｐｈｏｔｏｖｏｌｔａｉｃａｎｄｒｅｆｏｃｕｓｉｎｇｆｉｅｌｄｓｇｅｎｅｒａｔｅｄｂｙｔｈｅｂｅａｍｉｔｓｅｌｆ.


Acta Physica Sinica. 2002 51(1): 153-158. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 153-158. article doi:10.7498/aps.51.153 10.7498/aps.51.153 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.153 153-158 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.159

Ｔｈｅｑｕａｎｔｕｍｗａｖｅｆｕｎｃｔｉｏｎａｎｄｔｈｅｃｏｒｒｅｓｐｏｎｄｉｎｇｅｎｅｒｇｙｌｅｖｅｌｓｏｆｔｈｅｄｉｓｓｉｐａｔｉｖｅｍｅｓｏｓｃｏｐｉｃｃａｐａｃｉｔａｎｃｅｃｏｕｐｌｉｎｇｃｉｒｃｕｉｔｓａｒｅｏｂｔａｉｎｅｄｂｙｕｓｉｎｇｕｎｉｔａｒｙａｎｄｌｉｎｅａｒｔｒａｎｓｆｏｒｍａｔｉｏｎｓ.Ｔｈｅｑｕａｎｔｕｍｆｌｕｃｔｕａｔｉｏｎｏｆｃｈａｒｇｅａｎｄｃｕｒｒｅｎｔｉｎａｎａｒｂｉｔｒａｒｙｅｉｇｅｎｓｔａｔｅｏｆｔｈｅｓｙｓｔｅｍｈａｖｅｂｅｅｎａｌｓｏｇｉｖｅｎ.Ｔｈｅｒｅｓｕｌｔｓｓｈｏｗｔｈａｔｔｈｅｆｌｕｃｔｕａｔｉｏｎｏｆｃｈａｒｇｅａｎｄｃｕｒｒｅｎｔｄｅｐｅｎｄｓｏｎｎｏｔｏｎｌｙｔｈｅｅｉｇｅｎｓｔａｔｅｂｕｔａｌｓｏｔｈｅｅｌｅｃｔｒｏｎｉｃｄｅｖｉｃｅｐａｒａｍｅｔｅｒｓ.


Acta Physica Sinica. 2002 51(1): 159-162. Published 2005-04-11 ]]>

Ｔｈｅｑｕａｎｔｕｍｗａｖｅｆｕｎｃｔｉｏｎａｎｄｔｈｅｃｏｒｒｅｓｐｏｎｄｉｎｇｅｎｅｒｇｙｌｅｖｅｌｓｏｆｔｈｅｄｉｓｓｉｐａｔｉｖｅｍｅｓｏｓｃｏｐｉｃｃａｐａｃｉｔａｎｃｅｃｏｕｐｌｉｎｇｃｉｒｃｕｉｔｓａｒｅｏｂｔａｉｎｅｄｂｙｕｓｉｎｇｕｎｉｔａｒｙａｎｄｌｉｎｅａｒｔｒａｎｓｆｏｒｍａｔｉｏｎｓ.Ｔｈｅｑｕａｎｔｕｍｆｌｕｃｔｕａｔｉｏｎｏｆｃｈａｒｇｅａｎｄｃｕｒｒｅｎｔｉｎａｎａｒｂｉｔｒａｒｙｅｉｇｅｎｓｔａｔｅｏｆｔｈｅｓｙｓｔｅｍｈａｖｅｂｅｅｎａｌｓｏｇｉｖｅｎ.Ｔｈｅｒｅｓｕｌｔｓｓｈｏｗｔｈａｔｔｈｅｆｌｕｃｔｕａｔｉｏｎｏｆｃｈａｒｇｅａｎｄｃｕｒｒｅｎｔｄｅｐｅｎｄｓｏｎｎｏｔｏｎｌｙｔｈｅｅｉｇｅｎｓｔａｔｅｂｕｔａｌｓｏｔｈｅｅｌｅｃｔｒｏｎｉｃｄｅｖｉｃｅｐａｒａｍｅｔｅｒｓ.


Acta Physica Sinica. 2002 51(1): 159-162. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 159-162. article doi:10.7498/aps.51.159 10.7498/aps.51.159 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.159 159-162 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.163

Ｔｈｉｓｐａｐｅｒｐｒｅｓｅｎｔｓａｎｅｘｐｅｒｉｍｅｎｔａｌｍｅｔｈｏｄｆｏｒｍｅａｓｕｒｉｎｇｔｈｅｄｅｎｓｉｔｙｏｆｔｒａｐｐｉｎｇｃｈａｒｇｅｓ.Ｔｈｉｓｍｅｔｈｏｄｉｓｂａｓｅｄｏｎｔｈｅｄｙ ｎａｍｉｃｅｑｕｉｌｉｂｒｉｕｍｅｑｕａｔｉｏｎｆｏｒｔｈｅｐｒｏｃｅｓｓｏｆｔｒａｐｐｅｄｃｈａｒｇｅｓ.ＷｅｃａｎｏｂｔａｉｎｔｈｅｄｅｎｓｉｔｙａｎｄｔｈｅｌｏｃａｔｉｏｎｏｆｔｒａｐｐｉｎｇｃｈａｒｇｅｓｂｙｍｅａｓｕｒｉｎｇｔｈｅｈｉｇｈｆｒｅｑｕｅｎｃｙＣ ＶｃｕｒｖｅｏｆＭＯＳｃａｐａｃｉｔａｎｃｅｂｅｆｏｒｅａｎｄａｆｔｅｒｓｔｒｅｓｓ,ａｎｄｔｈｅｃｈａｎｇｅｏｆｇａｔｅｖｏｌｔａｇｅｕｎｄｅｒｃｏｎｓｔａｎｔｃｕｒｒｅｎｔｓｔｒｅｓｓ.Ｔｈｅａｎａｌｙｔｉｃａｌｅｘｐｒｅｓｓｉｏｎｏｆｔｈｅｄｅｎｓｉｔｙｏｆｔｒａｐｐｉｎｇｃｈａｒｇｅｓｉｓｐｒｏｐｏｓｅｄ .Ｔｈｅｍｅｔｈｏｄａｎｄｔｈｅｒｅｓｕｌｔｓｏｆｐａｒａｍｅｔｅｒｓｅｘｔｒａｃｔｉｏｎａｒｅａｌｓｏｐｒｅｓｅｎｔｅｄ .Ｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｓｓｈｏｗｔｈａｔｔｈｉｓｍｅｔｈｏｄｉｓｃｏｎｖｅｎｉｅｎｔａｎｄｐｒｅｃｉｓｅ .


Acta Physica Sinica. 2002 51(1): 163-166. Published 2005-04-11 ]]>

Ｔｈｉｓｐａｐｅｒｐｒｅｓｅｎｔｓａｎｅｘｐｅｒｉｍｅｎｔａｌｍｅｔｈｏｄｆｏｒｍｅａｓｕｒｉｎｇｔｈｅｄｅｎｓｉｔｙｏｆｔｒａｐｐｉｎｇｃｈａｒｇｅｓ.Ｔｈｉｓｍｅｔｈｏｄｉｓｂａｓｅｄｏｎｔｈｅｄｙ ｎａｍｉｃｅｑｕｉｌｉｂｒｉｕｍｅｑｕａｔｉｏｎｆｏｒｔｈｅｐｒｏｃｅｓｓｏｆｔｒａｐｐｅｄｃｈａｒｇｅｓ.ＷｅｃａｎｏｂｔａｉｎｔｈｅｄｅｎｓｉｔｙａｎｄｔｈｅｌｏｃａｔｉｏｎｏｆｔｒａｐｐｉｎｇｃｈａｒｇｅｓｂｙｍｅａｓｕｒｉｎｇｔｈｅｈｉｇｈｆｒｅｑｕｅｎｃｙＣ ＶｃｕｒｖｅｏｆＭＯＳｃａｐａｃｉｔａｎｃｅｂｅｆｏｒｅａｎｄａｆｔｅｒｓｔｒｅｓｓ,ａｎｄｔｈｅｃｈａｎｇｅｏｆｇａｔｅｖｏｌｔａｇｅｕｎｄｅｒｃｏｎｓｔａｎｔｃｕｒｒｅｎｔｓｔｒｅｓｓ.Ｔｈｅａｎａｌｙｔｉｃａｌｅｘｐｒｅｓｓｉｏｎｏｆｔｈｅｄｅｎｓｉｔｙｏｆｔｒａｐｐｉｎｇｃｈａｒｇｅｓｉｓｐｒｏｐｏｓｅｄ .Ｔｈｅｍｅｔｈｏｄａｎｄｔｈｅｒｅｓｕｌｔｓｏｆｐａｒａｍｅｔｅｒｓｅｘｔｒａｃｔｉｏｎａｒｅａｌｓｏｐｒｅｓｅｎｔｅｄ .Ｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｓｓｈｏｗｔｈａｔｔｈｉｓｍｅｔｈｏｄｉｓｃｏｎｖｅｎｉｅｎｔａｎｄｐｒｅｃｉｓｅ .


Acta Physica Sinica. 2002 51(1): 163-166. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 163-166. article doi:10.7498/aps.51.163 10.7498/aps.51.163 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.163 163-166 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.167

Ｉｎｍｅａｓｕｒｅｍｅｎｔｓｏｆｔｉｍｅｄｅｃａｙｉｎａｐｅｒｐｅｎｄｉｃｕｌａｒｄｏｕｂｌｅ ｌａｙｅｒｅｄｍｅｄｉｕｍ ,ａｌａｒｇｅｏｕｔｐｕｔｄｅｃａｙｗａｓｏｂｓｅｒｖｅｄｗｈｅｎａｒｅｇｕｌａｒｓｉｎｇｌｅ ｐｏｌｅｈｅａｄｗａｓｕｓｅｄｆｏｒｂｏｔｈｗｒｉｔｉｎｇａｎｄｒｅａｄｉｎｇ .Ｉｎｖｅｓｔｉｇａｔｉｏｎｓｏｆｔｈｉｓｐｈｅｎｏｍｅｎｏｎｒｅｖｅａｌｅｄｔｈａｔｔｈｅｄｅｍａｇｎｅｔｉｚａｔｉｏｎｏｆｔｈｅｍｅｄｉｕｍｗａｓｃａｕｓｅｄｂｙｔｈｅｉｎｓｔａｂｉｌｉｔｙｏｆｔｈｅｄｏｍａｉｎｗａｌｌｏｆｔｈｅｍａｉｎｐｏｌｅｆｉｌｍａｎｄａｌｓｏｂｙｔｈｅｃｏｎｃｅｎｔｒａｔｉｏｎｏｆｓｔｒａｙｆｉｅｌｄｓｂｙｔｈｅｍａｉｎｐｏｌｅｄｕｒｉｎｇｔｈｅｒｅａｄｉｎｇｐｒｏｃｅｓｓ.Ｓｅｖｅｒａｌｃｏｕｎｔｅｒｍｅａｓｕｒｅｓｗｅｒｅｐｒｏｐｏｓｅｄ .


Acta Physica Sinica. 2002 51(1): 167-170. Published 2005-04-11 ]]>

Ｉｎｍｅａｓｕｒｅｍｅｎｔｓｏｆｔｉｍｅｄｅｃａｙｉｎａｐｅｒｐｅｎｄｉｃｕｌａｒｄｏｕｂｌｅ ｌａｙｅｒｅｄｍｅｄｉｕｍ ,ａｌａｒｇｅｏｕｔｐｕｔｄｅｃａｙｗａｓｏｂｓｅｒｖｅｄｗｈｅｎａｒｅｇｕｌａｒｓｉｎｇｌｅ ｐｏｌｅｈｅａｄｗａｓｕｓｅｄｆｏｒｂｏｔｈｗｒｉｔｉｎｇａｎｄｒｅａｄｉｎｇ .Ｉｎｖｅｓｔｉｇａｔｉｏｎｓｏｆｔｈｉｓｐｈｅｎｏｍｅｎｏｎｒｅｖｅａｌｅｄｔｈａｔｔｈｅｄｅｍａｇｎｅｔｉｚａｔｉｏｎｏｆｔｈｅｍｅｄｉｕｍｗａｓｃａｕｓｅｄｂｙｔｈｅｉｎｓｔａｂｉｌｉｔｙｏｆｔｈｅｄｏｍａｉｎｗａｌｌｏｆｔｈｅｍａｉｎｐｏｌｅｆｉｌｍａｎｄａｌｓｏｂｙｔｈｅｃｏｎｃｅｎｔｒａｔｉｏｎｏｆｓｔｒａｙｆｉｅｌｄｓｂｙｔｈｅｍａｉｎｐｏｌｅｄｕｒｉｎｇｔｈｅｒｅａｄｉｎｇｐｒｏｃｅｓｓ.Ｓｅｖｅｒａｌｃｏｕｎｔｅｒｍｅａｓｕｒｅｓｗｅｒｅｐｒｏｐｏｓｅｄ .


Acta Physica Sinica. 2002 51(1): 167-170. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 167-170. article doi:10.7498/aps.51.167 10.7498/aps.51.167 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.167 167-170 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.171

ＩｎｏｒｄｅｒｔｏｏｂｔａｉｎｔｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｏｆｔｅｔｒａｇｏｎａｌｆｅｒｒｏｅｌｅｃｔｒｉｃPbFe0.5Nb0.5O3 ,ｗｅｃａｌｃｕｌａｔｅｄｉｔｓｔｏｔａｌｅｎｅｒｇｙｂｙｆｕｌｌ ｐｏｔｅｎｔｉａｌｌｉｎｅａｒｉｚｅｄａｕｇｍｅｎｔｅｄｐｌａｎｅｗａｖｅｍｅｔｈｏｄ .ＴｈｅｅｑｕｉｌｉｂｒｉｕｍｃｏｎｆｉｇｕｒａｔｉｏｎｏｆＢ ｓｉｔｅｃａｔｉｏｎｓ(ＦｅａｎｄＮｂ)ｗａｓｄｅｔｅｒｍｉｎｅｄ .ＴｈｅｄｉｓｐｌａｃｅｍｅｎｔｏｆＦｅｉｏｎｓａｌｏｎｇ [0 0 1 ]ｄｉｒｅｃｔｉｏｎｉｎｔｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｉｓ0 .0 2 2ｎｍａｎｄｔｈａｔｏｆＮｂｉｏｎｓｉｓ0 .0020ｎｍ .Ｔｈｅｆｅｒｒｏｅｌｅｃ ｔｒｉｃｉｎｓｔａｂｉｌｉｔｙｒｅｓｕｌｔｓｍａｉｎｌｙｆｒｏｍｔｈｅｄｉｓｐｌａｃｅｍｅｎｔｏｆＦｅｉｏｎｓ.


Acta Physica Sinica. 2002 51(1): 171-173. Published 2005-04-11 ]]>

ＩｎｏｒｄｅｒｔｏｏｂｔａｉｎｔｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｏｆｔｅｔｒａｇｏｎａｌｆｅｒｒｏｅｌｅｃｔｒｉｃPbFe0.5Nb0.5O3 ,ｗｅｃａｌｃｕｌａｔｅｄｉｔｓｔｏｔａｌｅｎｅｒｇｙｂｙｆｕｌｌ ｐｏｔｅｎｔｉａｌｌｉｎｅａｒｉｚｅｄａｕｇｍｅｎｔｅｄｐｌａｎｅｗａｖｅｍｅｔｈｏｄ .ＴｈｅｅｑｕｉｌｉｂｒｉｕｍｃｏｎｆｉｇｕｒａｔｉｏｎｏｆＢ ｓｉｔｅｃａｔｉｏｎｓ(ＦｅａｎｄＮｂ)ｗａｓｄｅｔｅｒｍｉｎｅｄ .ＴｈｅｄｉｓｐｌａｃｅｍｅｎｔｏｆＦｅｉｏｎｓａｌｏｎｇ [0 0 1 ]ｄｉｒｅｃｔｉｏｎｉｎｔｈｅｆｉｎｅｓｔｒｕｃｔｕｒｅｉｓ0 .0 2 2ｎｍａｎｄｔｈａｔｏｆＮｂｉｏｎｓｉｓ0 .0020ｎｍ .Ｔｈｅｆｅｒｒｏｅｌｅｃ ｔｒｉｃｉｎｓｔａｂｉｌｉｔｙｒｅｓｕｌｔｓｍａｉｎｌｙｆｒｏｍｔｈｅｄｉｓｐｌａｃｅｍｅｎｔｏｆＦｅｉｏｎｓ.


Acta Physica Sinica. 2002 51(1): 171-173. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 171-173. article doi:10.7498/aps.51.171 10.7498/aps.51.171 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.171 171-173 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.174

Ｔｈｅｔｉｍｅ ｒｅｓｏｌｖｅｄｐｈｏｔｏｌｕｍｉｎｅｓｃｅｎｃｅ (ＴＲＰＬ)ｓｐｅｃｔｒａｏｆｏｒｄｅｒｅｄＧａ0 .5Ｉｎ0 . 5Ｐａｌｌｏｙｓｇｒｏｗｎｂｙｍｅｔａｌｏｒｇａｎｉｃｖａｐｏｒｐｈａｓｅｅｐｉｔａｘｙｗｅｒｅｉｎｖｅｓｔｉｇａｔｅｄ .Ｔｈｅｌｅａｓｔ ｓｑｕａｒｅｆｉｔｔｉｎｇｏｆｔｈｅｌｕｍｉｎｅｓｃｅｎｃｅｄｅｃａｙｓｐｅｃｔｒａｓｈｏｗｓｔｈａｔｔｈｅｒｅｅｘｉｓｔｔｗｏｅｘｐｏｎｅｎｔｉａｌｐｒｏｃｅｓｓｅｓ:ｆｏｒｔｈｅｑｕｉｃｋｐｒｏｃｅｓｓｔｈｅｌｉｆｅｔｉｍｅτ1 ｉｓａｂｏｕｔ1 2 8ｐｓ— 2 50ｐｓａｎｄ 1 86ｐｓ— 546ｐｓａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅａｎｄ77Ｋ ,ｒｅｓｐｅｃｔｉｖｅｌｙ;ａｎｄｆｏｒｔｈｅｓｌｏｗｐｒｏｃｅｓｓｔｈｅｌｉｆｅｔｉｍｅτ2 ｉｓ,ａｂｏｕｔ3 0 8ｐｓ— 1 83 2ｐｓ,ａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅａｎｄａｔ77Ｋ ,ａｓｌｏｎｇａｓｎａｎｏｓｅｃｏｎｄａｎｄｅｖｅｎｍｏｒｅｔｈａｎ 2 8ｎｓ.Ｔｈｅｓｈｏｒｔｌｉｆｅｔｉｍｅｐｒｏｃｅｓｓｂｅｌｏｎｇｓｔｏｔｈｅｒｅｃｏｍｂｉｎａｔｉｏｎｏｆｃａｒｒｉｅｒｓｉｎｔｈｅｏｒｄｅｒｅｄｄｏｍａｉｎｓ,ｃｏｒｒｅｓｐｏｎｄｉｎｇｔｏｔｈｅｈｉｇｈ ｅｎｅｒｇｙｐｅａｋｉｎｔｈｅＰＬｓｐｅｃｔｒａ.Ｔｈｅｌｏｎｇｌｉｆｅｔｉｍｅｐｒｏｃｅｓｓｃｏｒｒｅｓｐｏｎｄｓｔｏｔｈｅｌｏｗ ｅｎｅｒｇｙｐｅａｋｉｎｔｈｅＰＬｓｐｅｃｔｒａ.Ｔｈｅｓｔｒｏｎｇｅｘｃｉｔａｔｉｏｎｉｎｔｅｎｓｉｔｙｄｅｐｅｎｄｅｎｃｅｏｆτ2 ａｔａｆｉｘｅｄｅｎｅｒｇｙｉｎｄｉｃａｔｅｓｔｈａｔｔｈｅｌｏｎｇｌｉｆｅｔｉｍｅｐｒｏｃｅｓｓｃｏｕｌｄｎｏｔｂｅｅｘｐｌａｉｎｅｄｉｎｔｅｒｍｓｏｆｄｏｎｏｒ ａｃｃｅｐｔｏｒｐａｉｒ(ＤＡＰ) .Ｗｅａｔｔｒｉｂｕｔｅｔｈｅｅｍｉｓｓｉｏｎｔｏｔｈｅｒｅｃｏｍｂｉｎａｔｉｏｎｂｅｔｗｅｅｎｔｈｅｓｐａｔｉａｌｌｙｓｅｐａｒａｔｅｄｃｅｎｔｅｒｓｏｆｔｈｅｅｌｅｃｔｒｏｎｓｉｎｏｒｄｅｒｅｄｄｏｍａｉｎｓａｎｄｔｈｅｈｏｌｅｓｉｎｄｉｓｏｒｄｅｒｅｄｒｅｇｉｏｎｓ.ＴｈｅＴＲＰＬｓｐｅｃｔｒａａｔ77Ｋｅｘｈｉｂｉｔａｂｌｕｅ ｓｈｉｆｔｗｉｔｈｔｉｍｅｄｅｌａｙ ,ｉｎｄｉｃａｔｉｎｇｔｈａｔｔｈｅｃａｒｒｉｅｒｓｔｒａｎｓｆｅｒｆｒｏｍｄｉｓｏｒｄｅｒｅｄｒｅｇｉｏｎｓｔｏｏｒｄｅｒｅｄｄｏｍａｉｎｓ.


Acta Physica Sinica. 2002 51(1): 174-177. Published 2005-04-11 ]]>

Ｔｈｅｔｉｍｅ ｒｅｓｏｌｖｅｄｐｈｏｔｏｌｕｍｉｎｅｓｃｅｎｃｅ (ＴＲＰＬ)ｓｐｅｃｔｒａｏｆｏｒｄｅｒｅｄＧａ0 .5Ｉｎ0 . 5Ｐａｌｌｏｙｓｇｒｏｗｎｂｙｍｅｔａｌｏｒｇａｎｉｃｖａｐｏｒｐｈａｓｅｅｐｉｔａｘｙｗｅｒｅｉｎｖｅｓｔｉｇａｔｅｄ .Ｔｈｅｌｅａｓｔ ｓｑｕａｒｅｆｉｔｔｉｎｇｏｆｔｈｅｌｕｍｉｎｅｓｃｅｎｃｅｄｅｃａｙｓｐｅｃｔｒａｓｈｏｗｓｔｈａｔｔｈｅｒｅｅｘｉｓｔｔｗｏｅｘｐｏｎｅｎｔｉａｌｐｒｏｃｅｓｓｅｓ:ｆｏｒｔｈｅｑｕｉｃｋｐｒｏｃｅｓｓｔｈｅｌｉｆｅｔｉｍｅτ1 ｉｓａｂｏｕｔ1 2 8ｐｓ— 2 50ｐｓａｎｄ 1 86ｐｓ— 546ｐｓａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅａｎｄ77Ｋ ,ｒｅｓｐｅｃｔｉｖｅｌｙ;ａｎｄｆｏｒｔｈｅｓｌｏｗｐｒｏｃｅｓｓｔｈｅｌｉｆｅｔｉｍｅτ2 ｉｓ,ａｂｏｕｔ3 0 8ｐｓ— 1 83 2ｐｓ,ａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅａｎｄａｔ77Ｋ ,ａｓｌｏｎｇａｓｎａｎｏｓｅｃｏｎｄａｎｄｅｖｅｎｍｏｒｅｔｈａｎ 2 8ｎｓ.Ｔｈｅｓｈｏｒｔｌｉｆｅｔｉｍｅｐｒｏｃｅｓｓｂｅｌｏｎｇｓｔｏｔｈｅｒｅｃｏｍｂｉｎａｔｉｏｎｏｆｃａｒｒｉｅｒｓｉｎｔｈｅｏｒｄｅｒｅｄｄｏｍａｉｎｓ,ｃｏｒｒｅｓｐｏｎｄｉｎｇｔｏｔｈｅｈｉｇｈ ｅｎｅｒｇｙｐｅａｋｉｎｔｈｅＰＬｓｐｅｃｔｒａ.Ｔｈｅｌｏｎｇｌｉｆｅｔｉｍｅｐｒｏｃｅｓｓｃｏｒｒｅｓｐｏｎｄｓｔｏｔｈｅｌｏｗ ｅｎｅｒｇｙｐｅａｋｉｎｔｈｅＰＬｓｐｅｃｔｒａ.Ｔｈｅｓｔｒｏｎｇｅｘｃｉｔａｔｉｏｎｉｎｔｅｎｓｉｔｙｄｅｐｅｎｄｅｎｃｅｏｆτ2 ａｔａｆｉｘｅｄｅｎｅｒｇｙｉｎｄｉｃａｔｅｓｔｈａｔｔｈｅｌｏｎｇｌｉｆｅｔｉｍｅｐｒｏｃｅｓｓｃｏｕｌｄｎｏｔｂｅｅｘｐｌａｉｎｅｄｉｎｔｅｒｍｓｏｆｄｏｎｏｒ ａｃｃｅｐｔｏｒｐａｉｒ(ＤＡＰ) .Ｗｅａｔｔｒｉｂｕｔｅｔｈｅｅｍｉｓｓｉｏｎｔｏｔｈｅｒｅｃｏｍｂｉｎａｔｉｏｎｂｅｔｗｅｅｎｔｈｅｓｐａｔｉａｌｌｙｓｅｐａｒａｔｅｄｃｅｎｔｅｒｓｏｆｔｈｅｅｌｅｃｔｒｏｎｓｉｎｏｒｄｅｒｅｄｄｏｍａｉｎｓａｎｄｔｈｅｈｏｌｅｓｉｎｄｉｓｏｒｄｅｒｅｄｒｅｇｉｏｎｓ.ＴｈｅＴＲＰＬｓｐｅｃｔｒａａｔ77Ｋｅｘｈｉｂｉｔａｂｌｕｅ ｓｈｉｆｔｗｉｔｈｔｉｍｅｄｅｌａｙ ,ｉｎｄｉｃａｔｉｎｇｔｈａｔｔｈｅｃａｒｒｉｅｒｓｔｒａｎｓｆｅｒｆｒｏｍｄｉｓｏｒｄｅｒｅｄｒｅｇｉｏｎｓｔｏｏｒｄｅｒｅｄｄｏｍａｉｎｓ.


Acta Physica Sinica. 2002 51(1): 174-177. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 174-177. article doi:10.7498/aps.51.174 10.7498/aps.51.174 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.174 174-177 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.178

ＴｈｅＧｅＯ2 ＳｉＯ2 ｇｅｌ ｇｌａｓｓｅｓｗｅｒｅｐｒｅｐａｒｅｄｂｙｔｈｅｓｏｌ ｇｅｌｍｅｔｈｏｄｗｉｔｈｔｅｔｒａｅｔｈｏｘｙｓｉｌａｎｅ (Ｓｉ(ＯＣ2 Ｈ5) 4)ａｎｄ 3 ｔｒｉｃｈｌｏｒｏｇｅｒ ｍａｎｉｕｍｐｒｏｐａｎｏｉｃａｃｉ (Ｃｌ3 ＧｅＣＨ2 ＣＨ2 ＣＯＯＨ)ａｓｓｔａｒｔｉｎｇｍａｔｅｒｉａｌｓ.Ｔｈｅｇｅｌ ｇｌａｓｓｅｓｓｈｏｗａｓｔｒｏｎｇｒｏｏｍ ｔｅｍｐｅｒａｔｕｒｅｐｈｏｔｏｌｕｍｉｎｅｓｃｅｎｃｅｗｉｔｈｐｅａｋｓａｔ575ａｎｄ 62 4ｎｍｕｎｄｅｒｔｈｅｅｘｃｉｔａｔｉｏｎｏｆｔｈｅ 53 2ｎｍｌｉｎｅｏｆａＮｄ∶ＹＡＧｌａｓｅｒ.ＴｈｅｐｈｏｔｏｌｕｍｉｎｅｓｃｅｎｃｅｓｐｅｃｔｒａａｒｅｃａｕｓｅｄｂｙＧｅＯ2 ｎａｎｏｐａｒｔｉｃｌｅｓｅｍｂｅｄｄｅｄｉｎｇｅｌ ｇｌａｓｓｅｓ.ＴｈｅＧｅＯ2 ＳｉＯ2 ｇｅｌ ｇｌａｓｓｅｓａｒｅｃｈａｒａｃｔｅｒｉｚｅｄｂｙｔｈｅｏｐｔｉｃａｌａｂｓｏｒｐｔｉｏｎ,Ｘ ｒａｙｄｉｆｆｒａｃｔｉｏｎ (ＸＲＤ)ａｎｄｔｒａｎｓｍｉｓｓｉｏｎｅｌｅｃｔｉｏｎｍｅｃｒｏｓｃｏｐｙ.ＴｈｅｓｉｚｅｏｆＧｅＯ2 ｎａｎｏｐａｒｔｉｃｌｅｓｅｍｂｅｄｄｅｄｉｎｇｅｌｇｌａｓｓｅｓｂｅｃｏｍｅｓｌａｒｇｅｒａｓｔｈｅＧｅＯ2 ｃｏｎｔｅｎｔｉｎｃｒｅａｓｅｓ,ａｎｄｔｈｕｓｔｈｅｏｐｔｉｃａｌａｂｓｏｒｐｔｉｏｎｅｄｇｅｏｆｔｈｅｇｅｌ ｇｌａｓｓｓｈｉｆｔｓｔｏｔｈｅｌｏｗｅｒ ｅｎｅｒｇｙｓｉｄｅ .ＴｈｅＧｅＯ2 ｎａｎｏｐａｒｔｉｃｌｅｓｔｒｕｃｔｕｒｅｓａｒｅｆｏｕｎｄｔｏｂｅａｍｏｒｐｈｏｕｓＧｅＯ2 ｉｎｔｈｅｇｅｌ ｇｌａｓｓｅｓｂｙｔｈｅＸＲＤａｎｄｔｈｅｅｌｅｃｔｒｏｎｄｉｆｆｒａｃｔｉｏｎｐａｔｔｅｒｎ .


Acta Physica Sinica. 2002 51(1): 178-182. Published 2005-04-11 ]]>

ＴｈｅＧｅＯ2 ＳｉＯ2 ｇｅｌ ｇｌａｓｓｅｓｗｅｒｅｐｒｅｐａｒｅｄｂｙｔｈｅｓｏｌ ｇｅｌｍｅｔｈｏｄｗｉｔｈｔｅｔｒａｅｔｈｏｘｙｓｉｌａｎｅ (Ｓｉ(ＯＣ2 Ｈ5) 4)ａｎｄ 3 ｔｒｉｃｈｌｏｒｏｇｅｒ ｍａｎｉｕｍｐｒｏｐａｎｏｉｃａｃｉ (Ｃｌ3 ＧｅＣＨ2 ＣＨ2 ＣＯＯＨ)ａｓｓｔａｒｔｉｎｇｍａｔｅｒｉａｌｓ.Ｔｈｅｇｅｌ ｇｌａｓｓｅｓｓｈｏｗａｓｔｒｏｎｇｒｏｏｍ ｔｅｍｐｅｒａｔｕｒｅｐｈｏｔｏｌｕｍｉｎｅｓｃｅｎｃｅｗｉｔｈｐｅａｋｓａｔ575ａｎｄ 62 4ｎｍｕｎｄｅｒｔｈｅｅｘｃｉｔａｔｉｏｎｏｆｔｈｅ 53 2ｎｍｌｉｎｅｏｆａＮｄ∶ＹＡＧｌａｓｅｒ.ＴｈｅｐｈｏｔｏｌｕｍｉｎｅｓｃｅｎｃｅｓｐｅｃｔｒａａｒｅｃａｕｓｅｄｂｙＧｅＯ2 ｎａｎｏｐａｒｔｉｃｌｅｓｅｍｂｅｄｄｅｄｉｎｇｅｌ ｇｌａｓｓｅｓ.ＴｈｅＧｅＯ2 ＳｉＯ2 ｇｅｌ ｇｌａｓｓｅｓａｒｅｃｈａｒａｃｔｅｒｉｚｅｄｂｙｔｈｅｏｐｔｉｃａｌａｂｓｏｒｐｔｉｏｎ,Ｘ ｒａｙｄｉｆｆｒａｃｔｉｏｎ (ＸＲＤ)ａｎｄｔｒａｎｓｍｉｓｓｉｏｎｅｌｅｃｔｉｏｎｍｅｃｒｏｓｃｏｐｙ.ＴｈｅｓｉｚｅｏｆＧｅＯ2 ｎａｎｏｐａｒｔｉｃｌｅｓｅｍｂｅｄｄｅｄｉｎｇｅｌｇｌａｓｓｅｓｂｅｃｏｍｅｓｌａｒｇｅｒａｓｔｈｅＧｅＯ2 ｃｏｎｔｅｎｔｉｎｃｒｅａｓｅｓ,ａｎｄｔｈｕｓｔｈｅｏｐｔｉｃａｌａｂｓｏｒｐｔｉｏｎｅｄｇｅｏｆｔｈｅｇｅｌ ｇｌａｓｓｓｈｉｆｔｓｔｏｔｈｅｌｏｗｅｒ ｅｎｅｒｇｙｓｉｄｅ .ＴｈｅＧｅＯ2 ｎａｎｏｐａｒｔｉｃｌｅｓｔｒｕｃｔｕｒｅｓａｒｅｆｏｕｎｄｔｏｂｅａｍｏｒｐｈｏｕｓＧｅＯ2 ｉｎｔｈｅｇｅｌ ｇｌａｓｓｅｓｂｙｔｈｅＸＲＤａｎｄｔｈｅｅｌｅｃｔｒｏｎｄｉｆｆｒａｃｔｉｏｎｐａｔｔｅｒｎ .


Acta Physica Sinica. 2002 51(1): 178-182. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 178-182. article doi:10.7498/aps.51.178 10.7498/aps.51.178 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.178 178-182 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.183

ＮａｎｏｃｒｙｓｔａｌｌｉｎｅＧａＳｂＰａｒｔｉｃｌｅｓｅｍｂｅｄｄｅｄｉｎＳｉＯ2 ｆｉｌｍｓｗｅｒｅｇｒｏｗｎｂｙｒａｄｉｏｆｒｅｑｕｅｎｃｙｍａｇｎｅｔｒｏｎｃｏ ｓｐｕｔｔｅｒｉｎｇ .ＴｈｅｔｒａｎｓｍｉｓｓｉｏｎａｂｓｏｒｐｔｉｏｎｏｆｔｈｅｃｏｍｐｏｓｉｔｅｆｉｌｍｗａｓｒｅｃｏｒｄｅｄｗｉｔｈＣａｒｙ 5Ｅｓｐｅｃｔｒｏｐｈｏｔｏｍｅｔｅｒａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅ.Ｔｈｅｔｗｏ ｐｈｏｔｏｎｏｐｔｉｃａｌｎｏｎｌｉｎｅａｒｉｔｉｅｓｏｆｔｈｅＧａＳｂ ＳｉＯ2 ｃｏｍｐｏｓｉｔｅｔｈｉｎｆｉｌｍｓａｔ63 2 .8ｎｍｗｅｒｅｍｅａｓｕｒｅｄｂｙＺ ｓｃａｎｍｅｔｈｏｄ,ａｎｄｔｈｅｒｅｓｕｌｔｓａｒｅ:ｔｗｏｐｈｏｔｏｎａｂｓｏｒｐｔｉｏｎｃｏｅｆｆｉｃｉｅｎｔβ≈ 0 . 0 82ｍ Ｗ ,ｎｏｎｌｉｎｅａｒｒｅｆｒａｃｔｉｖｅｉｎｄｅｘγ≈ 3 .76× 1 0 -9ｍ2 Ｗａｎｄｔｈｅｎｏｎｌｉｎｅａｒｓｕｓｃｅｐｔｉｂｉｌｉｔｙχ(3 )≈ 7.84× 1 0 -9ｅｓｕ .


Acta Physica Sinica. 2002 51(1): 183-186. Published 2005-04-11 ]]>

ＮａｎｏｃｒｙｓｔａｌｌｉｎｅＧａＳｂＰａｒｔｉｃｌｅｓｅｍｂｅｄｄｅｄｉｎＳｉＯ2 ｆｉｌｍｓｗｅｒｅｇｒｏｗｎｂｙｒａｄｉｏｆｒｅｑｕｅｎｃｙｍａｇｎｅｔｒｏｎｃｏ ｓｐｕｔｔｅｒｉｎｇ .ＴｈｅｔｒａｎｓｍｉｓｓｉｏｎａｂｓｏｒｐｔｉｏｎｏｆｔｈｅｃｏｍｐｏｓｉｔｅｆｉｌｍｗａｓｒｅｃｏｒｄｅｄｗｉｔｈＣａｒｙ 5Ｅｓｐｅｃｔｒｏｐｈｏｔｏｍｅｔｅｒａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅ.Ｔｈｅｔｗｏ ｐｈｏｔｏｎｏｐｔｉｃａｌｎｏｎｌｉｎｅａｒｉｔｉｅｓｏｆｔｈｅＧａＳｂ ＳｉＯ2 ｃｏｍｐｏｓｉｔｅｔｈｉｎｆｉｌｍｓａｔ63 2 .8ｎｍｗｅｒｅｍｅａｓｕｒｅｄｂｙＺ ｓｃａｎｍｅｔｈｏｄ,ａｎｄｔｈｅｒｅｓｕｌｔｓａｒｅ:ｔｗｏｐｈｏｔｏｎａｂｓｏｒｐｔｉｏｎｃｏｅｆｆｉｃｉｅｎｔβ≈ 0 . 0 82ｍ Ｗ ,ｎｏｎｌｉｎｅａｒｒｅｆｒａｃｔｉｖｅｉｎｄｅｘγ≈ 3 .76× 1 0 -9ｍ2 Ｗａｎｄｔｈｅｎｏｎｌｉｎｅａｒｓｕｓｃｅｐｔｉｂｉｌｉｔｙχ(3 )≈ 7.84× 1 0 -9ｅｓｕ .


Acta Physica Sinica. 2002 51(1): 183-186. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 183-186. article doi:10.7498/aps.51.183 10.7498/aps.51.183 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.183 183-186 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.187

ＯｐｔｉｃａｌｌｙｔｒａｎｓｐａｒｅｎｔＳｂ ｄｏｐｅｄＳｒＴｉＯ3 (SrTi1-xSbxO3 )ｔｈｉｎｆｉｌｍｓｗｉｔｈａｔｒａｎｓｍｉｔｔａｎｃｅｈｉｇｈｅｒｔｈａｎ 90 %ｉｎｖｉｓｉｂｌｅｒｅｇｉｏｎｈａｖｅｂｅｅｎｇｒｏｗｎｏｎＳｒＴｉＯ3 (0 0 1 )ｓｕｂｓｔｒａｔｅｓｂｙｐｕｌｓｅｄｌａｓｅｒｄｅｐｏｓｉｔｉｏｎｍｅｔｈｏｄｕｓｉｎｇａｎＸｅＣｌｌａｓｅｒｕｎｄｅｒｏｘｙｇｅｎｐａｒｔｉａｌｐｒｅｓｓｕｒｅｏｆ2 0Ｐａ.ＴｈｅｔｈｉｎｆｉｌｍｗｉｔｈＳｂｄｏｐｉｎｇｃｏｎｃｅｎｔｒａｔｉｏｎｏｆｘ=0 .0 5ｓｈｏｗｓｍｅｔａｌｌｉｃ ｌｉｋｅｃｏｎｄｕｃｔｉｖｉｔｙｗｉｔｈａｒｅｓｉｓｔｉｖｉｔｙρ～ 6.99×1 0 -3 Ω·ｃｍａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅ.ＸＰＳａｎｄｓｙｎｃｈｒｏｔｒｏｎｒａｄｉａｔｉｏｎｐｈｏｔｏｅｌｅｃｔｒｏｎｓｐｅｃｔｒｏｓｃｏｐｙ (ＳＲ ＰＥＳ)ｍｅａｓｕｒｅｍｅｎｔｆｒｏｍｔｈｅＳｒＴｉ0 . 95Ｓｂ0 .0 5Ｏ3 ｔｈｉｎｆｉｌｍｒｅｖｅａｌｓｔｈａｔｔｈｅｓｈａｌｌｏｗａｎｄｄｅｅｐｉｍｐｕｒｉｔｙｄｏｎｏｒｌｅｖｅｌｓｗｉｔｈｉｎｔｈｅｂａｎｄｇａｐｏｆｔｈｅｐａｒｅｎｔｃｏｍｐｏｕｎｄＳｒＴｉＯ3 ａｒｅｉｎｄｕｃｅｄｂｙｔｈｅＳｂｄｏｐｉｎｇ.ＴｈｅｄｅｌｏｃａｌｉｚｅｄｅｌｅｃｔｒｏｎｓｗｉｔｈｉｎｔｈｅｓｈａｌｌｏｗｌｅｖｅｌｓｎｅａｒｔｈｅＦｅｒｍｉｌｅｖｅｌｃａｎｂｅｅｘｃｉｔｅｄｔｏｔｈｅｃｏｎｄｕｃｔｉｏｎｂａｎｄａｓｆｒｅｅｃａｒｒｉｅｒｓｆｏｒｅｌｅｃｔｒｉｃａｌｃｏｎｄｕｃｔｉｏｎｂｙｔｈｅｒｍａｌｉｏｎｉｚａｔｉｏｎ.Ｔｈｅｗｉｄｅｂａｎｄｇａｐ ,ｓｍａｌｌｔｒａｎｓｉｔｉｏｎｐｒｏｂａｂｉｌｉｔｙａｎｄｗｅａｋａｂｓｏｒｐｔｉｏｎｄｕｅｔｏｔｈｅｌｏｗｄｅｎｓｉｔｙｏｆｓｔａｔｅｓｉｎｔｈｅｉｍｐｕｒｉｔｙｌｅｖｅｌｓｒｅｓｕｌｔｉｎｔｈｅｏｐｔｉｃａｌｔｒａｎｓｐａｒｅｎｃｙｏｆｔｈｅｆｉｌｍ .


Acta Physica Sinica. 2002 51(1): 187-191. Published 2005-04-11 ]]>

ＯｐｔｉｃａｌｌｙｔｒａｎｓｐａｒｅｎｔＳｂ ｄｏｐｅｄＳｒＴｉＯ3 (SrTi1-xSbxO3 )ｔｈｉｎｆｉｌｍｓｗｉｔｈａｔｒａｎｓｍｉｔｔａｎｃｅｈｉｇｈｅｒｔｈａｎ 90 %ｉｎｖｉｓｉｂｌｅｒｅｇｉｏｎｈａｖｅｂｅｅｎｇｒｏｗｎｏｎＳｒＴｉＯ3 (0 0 1 )ｓｕｂｓｔｒａｔｅｓｂｙｐｕｌｓｅｄｌａｓｅｒｄｅｐｏｓｉｔｉｏｎｍｅｔｈｏｄｕｓｉｎｇａｎＸｅＣｌｌａｓｅｒｕｎｄｅｒｏｘｙｇｅｎｐａｒｔｉａｌｐｒｅｓｓｕｒｅｏｆ2 0Ｐａ.ＴｈｅｔｈｉｎｆｉｌｍｗｉｔｈＳｂｄｏｐｉｎｇｃｏｎｃｅｎｔｒａｔｉｏｎｏｆｘ=0 .0 5ｓｈｏｗｓｍｅｔａｌｌｉｃ ｌｉｋｅｃｏｎｄｕｃｔｉｖｉｔｙｗｉｔｈａｒｅｓｉｓｔｉｖｉｔｙρ～ 6.99×1 0 -3 Ω·ｃｍａｔｒｏｏｍｔｅｍｐｅｒａｔｕｒｅ.ＸＰＳａｎｄｓｙｎｃｈｒｏｔｒｏｎｒａｄｉａｔｉｏｎｐｈｏｔｏｅｌｅｃｔｒｏｎｓｐｅｃｔｒｏｓｃｏｐｙ (ＳＲ ＰＥＳ)ｍｅａｓｕｒｅｍｅｎｔｆｒｏｍｔｈｅＳｒＴｉ0 . 95Ｓｂ0 .0 5Ｏ3 ｔｈｉｎｆｉｌｍｒｅｖｅａｌｓｔｈａｔｔｈｅｓｈａｌｌｏｗａｎｄｄｅｅｐｉｍｐｕｒｉｔｙｄｏｎｏｒｌｅｖｅｌｓｗｉｔｈｉｎｔｈｅｂａｎｄｇａｐｏｆｔｈｅｐａｒｅｎｔｃｏｍｐｏｕｎｄＳｒＴｉＯ3 ａｒｅｉｎｄｕｃｅｄｂｙｔｈｅＳｂｄｏｐｉｎｇ.ＴｈｅｄｅｌｏｃａｌｉｚｅｄｅｌｅｃｔｒｏｎｓｗｉｔｈｉｎｔｈｅｓｈａｌｌｏｗｌｅｖｅｌｓｎｅａｒｔｈｅＦｅｒｍｉｌｅｖｅｌｃａｎｂｅｅｘｃｉｔｅｄｔｏｔｈｅｃｏｎｄｕｃｔｉｏｎｂａｎｄａｓｆｒｅｅｃａｒｒｉｅｒｓｆｏｒｅｌｅｃｔｒｉｃａｌｃｏｎｄｕｃｔｉｏｎｂｙｔｈｅｒｍａｌｉｏｎｉｚａｔｉｏｎ.Ｔｈｅｗｉｄｅｂａｎｄｇａｐ ,ｓｍａｌｌｔｒａｎｓｉｔｉｏｎｐｒｏｂａｂｉｌｉｔｙａｎｄｗｅａｋａｂｓｏｒｐｔｉｏｎｄｕｅｔｏｔｈｅｌｏｗｄｅｎｓｉｔｙｏｆｓｔａｔｅｓｉｎｔｈｅｉｍｐｕｒｉｔｙｌｅｖｅｌｓｒｅｓｕｌｔｉｎｔｈｅｏｐｔｉｃａｌｔｒａｎｓｐａｒｅｎｃｙｏｆｔｈｅｆｉｌｍ .


Acta Physica Sinica. 2002 51(1): 187-191. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 187-191. article doi:10.7498/aps.51.187 10.7498/aps.51.187 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.187 187-191 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.192

Ｔｈｅｄｏｍａｉｎｒｅｖｅｒｓａｌｃｈａｒａｃｔｅｒｉｓｔｉｃｓｏｆｎｅａｒ ｓｔｏｉｃｈｉｏｍｅｔｒｉｃＬｉＮｂＯ3 ｓｉｎｇｌｅｃｒｙｓｔａｌｓ,ｗｈｉｃｈｗｅｒｅｐｒｅｐａｒｅｄｂｙｔｈｅＣｚｏｃｈｒａｌｓｋｉｍｅｔｈｏｄｗｉｔｈＫ2 Ｏｆｌｕｘａｎｄｔｈｅｖａｐｏｒｔｒａｎｓｐｏｒｔｅｑｕｉｌｉｂｒａｔｉｏｎ,ｗｅｒｅｉｎｖｅｓｔｉｇａｔｅｄ.Ｔｈｅｒｅｓｕｌｔｓｓｈｏｗｔｈａｔｔｈｅｓｗｉｔｃｈｆｉｅｌｄｆｏｒ1 80°ｆｅｒｒｏｅｌｅｃｔｒｉｃｄｏｍａｉｎｒｅｖｅｒｓａｌｉｎｔｈｅｎｅａｒ ｓｔｏｉｃｈｉｏｍｅｎｔＬｉＮｂＯ3 ｃｒｙｓｔａｌｄｅｃｒｅａｓｅｓｗｉｔｈ [Ｌｉ] [Ｎｂ]ｒａｔｉｏ.Ｗｅｓｕｃｃｅｓｓｆｕｌｌｙａｃｈｉｅｖｅｄ1 80°ｄｏｍａｉｎｒｅｖｅｒｓａｌｉｎｔｈｅｎｅａｒ ｓｔｏｉｃｈｉｏｍｅｔｒｉｃＬｉＮｂＯ3 ｓａｍｐｌｅｓｏｆ1 . 0ｍｍｔｈｉｃｋｎｅｓｓｂｙｕｓｉｎｇａ4. 0ｋＶ ｍｍｓｗｉｔｃｈｆｉｅｌｄ .ＡｐｒｅｌｉｍｉｎａｒｙｅｘｐｌａｎａｔｉｏｎｆｏｒｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｓｉｓｇｉｖｅｎｂａｓｅｄｏｎｔｈｅＬｉ ｓｉｔｅｖａｃａｎｃｙｐｏｉｎｔｄｅｆｅｃｔｍｏｄｅｌ.


Acta Physica Sinica. 2002 51(1): 192-196. Published 2005-04-11 ]]>

Ｔｈｅｄｏｍａｉｎｒｅｖｅｒｓａｌｃｈａｒａｃｔｅｒｉｓｔｉｃｓｏｆｎｅａｒ ｓｔｏｉｃｈｉｏｍｅｔｒｉｃＬｉＮｂＯ3 ｓｉｎｇｌｅｃｒｙｓｔａｌｓ,ｗｈｉｃｈｗｅｒｅｐｒｅｐａｒｅｄｂｙｔｈｅＣｚｏｃｈｒａｌｓｋｉｍｅｔｈｏｄｗｉｔｈＫ2 Ｏｆｌｕｘａｎｄｔｈｅｖａｐｏｒｔｒａｎｓｐｏｒｔｅｑｕｉｌｉｂｒａｔｉｏｎ,ｗｅｒｅｉｎｖｅｓｔｉｇａｔｅｄ.Ｔｈｅｒｅｓｕｌｔｓｓｈｏｗｔｈａｔｔｈｅｓｗｉｔｃｈｆｉｅｌｄｆｏｒ1 80°ｆｅｒｒｏｅｌｅｃｔｒｉｃｄｏｍａｉｎｒｅｖｅｒｓａｌｉｎｔｈｅｎｅａｒ ｓｔｏｉｃｈｉｏｍｅｎｔＬｉＮｂＯ3 ｃｒｙｓｔａｌｄｅｃｒｅａｓｅｓｗｉｔｈ [Ｌｉ] [Ｎｂ]ｒａｔｉｏ.Ｗｅｓｕｃｃｅｓｓｆｕｌｌｙａｃｈｉｅｖｅｄ1 80°ｄｏｍａｉｎｒｅｖｅｒｓａｌｉｎｔｈｅｎｅａｒ ｓｔｏｉｃｈｉｏｍｅｔｒｉｃＬｉＮｂＯ3 ｓａｍｐｌｅｓｏｆ1 . 0ｍｍｔｈｉｃｋｎｅｓｓｂｙｕｓｉｎｇａ4. 0ｋＶ ｍｍｓｗｉｔｃｈｆｉｅｌｄ .ＡｐｒｅｌｉｍｉｎａｒｙｅｘｐｌａｎａｔｉｏｎｆｏｒｅｘｐｅｒｉｍｅｎｔａｌｒｅｓｕｌｔｓｉｓｇｉｖｅｎｂａｓｅｄｏｎｔｈｅＬｉ ｓｉｔｅｖａｃａｎｃｙｐｏｉｎｔｄｅｆｅｃｔｍｏｄｅｌ.


Acta Physica Sinica. 2002 51(1): 192-196. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 192-196. article doi:10.7498/aps.51.192 10.7498/aps.51.192 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.192 192-196 <![CDATA[]]> //m.suprmerch.com/en/article/doi/10.7498/aps.51.197

ＴｈｅｃｏｌｌａｐｓｅｓｏｌｕｔｉｏｎｏｆａｓｔａｒｗｉｔｈｕｎｉｆｏｒｍｄｅｎｓｉｔｙａｎｄｚｅｒｏｐｒｅｓｓｕｒｅｇｉｖｅｎｉｎｔｈｅｃｌａｓｓｉｃｐａｐｅｒｏｆＯｐｐｅｎｈｅｉｍｅｒａｎｄＳｎｙｄｅｒｉｓｐｒｏｖｅｄｔｏｂｅｉｎｃｏｍｐｌｅｔｅ;ｉｔｃａｎｎｏｔｃｏｒｒｅｃｔｌｙｃｏｎｎｅｃｔｔｈｅＦｒｉｅｄｍａｎｎａｎｄＳｃｈｗａｒｚｓｃｈｉｌｄｍｅｔｒｉｃｓａｓｔｈｅｉｎｔｅｒｉｏｒａｎｄｅｘｔｅｒｉｏｒｓｏｌｕｔｉｏｎｓ.Ｂｙｔｈｅｅｘｔｅｎｓｉｏｎｏｆｓｏｌｕｔｉｏｎｐａｒａｍｅｔｅｒｉｎｔｈｅｄｉｓｃｒｅｔｅｓｐａｃｅｔｉｍｅ,ｗｅｃｏｎｓｔｒｕｃｔａｃｏｍｐｌｅｔｅｇｒａｖｉｔａｔｉｏｎａｌｓｏｌｕｔｉｏｎ ,ｗｈｉｃｈｃｏｕｌｄｍａｋｅａｎｅｑｕｉｖａｌｅｎｃｅｃｏｎｎｅｃｔｉｏｎｂｅｔｗｅｅｎｔｈｅＦｒｉｅｄｍａｎｎａｎｄＳｃｈｗａｒｚｓｃｈｉｌｄｍｅｔｒｉｃｓａｎｄｉｓｐｒｏｖｅｓｔｏｂｅｓｉｎｇｕｌａｒｉｔｙ ｆｒｅｅ.Ｔｈｅｓｏｌｕｔｉｏｎｓｈｏｗｓｔｈａｔｔｈｅｒｅｅｘｉｓｔｓａｒｅｌａｔｉｏｎｓｈｉｐａｍｏｎｇｍａｔｔｅｒ,ｇｒａｖｉｔａｔｉｏｎａｎｄｄｉｓｃｒｅｔｅｓｐａｃｅｔｉｍｅｃｏｎｆｉｇｕｒａｔｉｏｎ .


Acta Physica Sinica. 2002 51(1): 197-200. Published 2005-04-11 ]]>

ＴｈｅｃｏｌｌａｐｓｅｓｏｌｕｔｉｏｎｏｆａｓｔａｒｗｉｔｈｕｎｉｆｏｒｍｄｅｎｓｉｔｙａｎｄｚｅｒｏｐｒｅｓｓｕｒｅｇｉｖｅｎｉｎｔｈｅｃｌａｓｓｉｃｐａｐｅｒｏｆＯｐｐｅｎｈｅｉｍｅｒａｎｄＳｎｙｄｅｒｉｓｐｒｏｖｅｄｔｏｂｅｉｎｃｏｍｐｌｅｔｅ;ｉｔｃａｎｎｏｔｃｏｒｒｅｃｔｌｙｃｏｎｎｅｃｔｔｈｅＦｒｉｅｄｍａｎｎａｎｄＳｃｈｗａｒｚｓｃｈｉｌｄｍｅｔｒｉｃｓａｓｔｈｅｉｎｔｅｒｉｏｒａｎｄｅｘｔｅｒｉｏｒｓｏｌｕｔｉｏｎｓ.Ｂｙｔｈｅｅｘｔｅｎｓｉｏｎｏｆｓｏｌｕｔｉｏｎｐａｒａｍｅｔｅｒｉｎｔｈｅｄｉｓｃｒｅｔｅｓｐａｃｅｔｉｍｅ,ｗｅｃｏｎｓｔｒｕｃｔａｃｏｍｐｌｅｔｅｇｒａｖｉｔａｔｉｏｎａｌｓｏｌｕｔｉｏｎ ,ｗｈｉｃｈｃｏｕｌｄｍａｋｅａｎｅｑｕｉｖａｌｅｎｃｅｃｏｎｎｅｃｔｉｏｎｂｅｔｗｅｅｎｔｈｅＦｒｉｅｄｍａｎｎａｎｄＳｃｈｗａｒｚｓｃｈｉｌｄｍｅｔｒｉｃｓａｎｄｉｓｐｒｏｖｅｓｔｏｂｅｓｉｎｇｕｌａｒｉｔｙ ｆｒｅｅ.Ｔｈｅｓｏｌｕｔｉｏｎｓｈｏｗｓｔｈａｔｔｈｅｒｅｅｘｉｓｔｓａｒｅｌａｔｉｏｎｓｈｉｐａｍｏｎｇｍａｔｔｅｒ,ｇｒａｖｉｔａｔｉｏｎａｎｄｄｉｓｃｒｅｔｅｓｐａｃｅｔｉｍｅｃｏｎｆｉｇｕｒａｔｉｏｎ .


Acta Physica Sinica. 2002 51(1): 197-200. Published 2005-04-11 ]]> 2002-01-05T00:00:00+00:00 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 2002 51(1): 197-200. article doi:10.7498/aps.51.197 10.7498/aps.51.197 Acta Physica Sinica 51 1 2005-04-11 //m.suprmerch.com/en/article/doi/10.7498/aps.51.197 197-200