| ²é¿´: 293 | »Ø¸´: 0 | ||
Jonesupermax½ð³æ (ÕýʽдÊÖ)
|
[ÇóÖú]
¹â»î»¯µÄרҵÊõÓïÀí½â
|
|
1. Due to moderate uncaging cross-sections (daUu where da is the absorption cross-section and Uu the uncaging quantum yield) described for the usual photoremovable groups, two-photon fluorescence uncaging, has been sparingly described in the literature by contrast to two-photon fluorescence excitation¡£ÆäÖУ¬ cross-sectionsÔõô½âÊÍ¡£ 2. A main difference between two-photon fluorescence uncaging and two-photon fluorescence excitation is that, in the former case, the excitation process will be independently triggered by standard excitation allowing subsequent biophysical experiments (single molecule fluorescence tracking, bleaching, etc.).Õâ¾ä»°ÍêÈ«²»Àí½â£¬ two-photon fluorescence uncagingºÍtwo-photon fluorescence excitationµÄÇø±ðµ½µ×ÔÚÄÄ£¿Çó´óÉñÏê½â |
» ²ÂÄãϲ»¶
²ÄÁϵ÷¼Á
ÒѾÓÐ3È˻ظ´
070300»¯Ñ§279Çóµ÷¼Á
ÒѾÓÐ4È˻ظ´
Ò»Ö¾Ô¸»ª¶«Àí¹¤085601²ÄÁϹ¤³Ì303·ÖÇóµ÷¼Á
ÒѾÓÐ14È˻ظ´
Èí¼þ¹¤³ÌÇóµ÷¼Á22Èí¹¤296·ÖÇóµ÷¼Á£¬½ÓÊÜ¿çµ÷
ÒѾÓÐ4È˻ظ´
²ÄÁϹ¤³Ì085601£¬270Çóµ÷¼Á
ÒѾÓÐ3È˻ظ´
288Çóµ÷¼Á£¬Ò»Ö¾Ô¸»ªÄÏÀí¹¤´óѧ071005
ÒѾÓÐ10È˻ظ´
085600²ÄÁÏÓ뻯¹¤×¨Ë¶329 Çóµ÷¼Á
ÒѾÓÐ20È˻ظ´
275Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
һ־Ըɽ¶«´óѧ»¯Ñ§Ó뻯¹¤Ñ§Ôº²ÄÁÏÓ뻯¹¤×¨Ë¶£¬360·ÖÇóµ÷¼Á
ÒѾÓÐ5È˻ظ´
±¾¿Æ211£¬293·ÖÇëÇóµ÷¼Á
ÒѾÓÐ11È˻ظ´
ÕÒµ½Ò»Ð©Ïà¹ØµÄ¾«»ªÌû×Ó£¬Ï£ÍûÓÐÓÃŶ~
µ°°×ÔÚÔÆÄ¸±íÃæµÄÎü¸½Á¦Ç¿Âð£¿
ÒѾÓÐ22È˻ظ´
ÖпÆÔº´óÁ¬»¯ÎïËùÐÁÇÚÑо¿Ô±Íâʽ»Á÷»Ø¹Ë
ÒѾÓÐ22È˻ظ´
´ß»¯¼ÁÔö´óÁËËÙÂʳ£Êýµ«Ã»Óиıä»î»¯ÄÜ-À´×Ôһƪ¾µäÎÄÏ×£¬ÈçºÎÀí½â£¿
ÒѾÓÐ3È˻ظ´
ÉúÎïÐÅϢѧרÌâ£ÉúÎï°æ£¬Ò½Ñ§°æºÍÐÅÏ¢¿ÆÑ§°æ¹²Í¬´´½¨
ÒѾÓÐ87È˻ظ´
¿ÆÑдÓСľ³æ¿ªÊ¼£¬ÈËÈËΪÎÒ£¬ÎÒΪÈËÈË














»Ø¸´´ËÂ¥
µã»÷ÕâÀïËÑË÷¸ü¶àÏà¹Ø×ÊÔ´