m |
m (→Papers to read) |
||
Line 1: | Line 1: | ||
= Papers to read = | = Papers to read = | ||
− | From {{thisday|31|December|2023}} onward, I'm starting the new "tradition" of keeping track of the papers I need to read. | + | From {{thisday|31|December|2023}} onward, {{I}}'m starting the new "tradition" of keeping track of the papers I need to read. By "read" I mean, really, "study" in some depth (skimming through a paper is the lot of the researcher). |
# {{wang19a}} Since 14:57 on {{thisday|31|December|2023}} | # {{wang19a}} Since 14:57 on {{thisday|31|December|2023}} | ||
# {{meuret15a}} Since 16:01 on {{thisday|31|December|2023}}, for their $1/N$ analysis of the [[antibunching]] of $N$ emitters. | # {{meuret15a}} Since 16:01 on {{thisday|31|December|2023}}, for their $1/N$ analysis of the [[antibunching]] of $N$ emitters. | ||
# {{boll20a}} Since 16:02 on {{thisday|31|December|2023}} for their flat $g^{(2)}(\tau)$ (see Fig. 3). | # {{boll20a}} Since 16:02 on {{thisday|31|December|2023}} for their flat $g^{(2)}(\tau)$ (see Fig. 3). | ||
− | |||
# {{brassard00a}} Since 16:17 on {{thisday|31|December|2023}} for SPDC being better than weak laser pulses (I'm interested in general in how weak laser pulses are useless [[SPS]] for QIP). | # {{brassard00a}} Since 16:17 on {{thisday|31|December|2023}} for SPDC being better than weak laser pulses (I'm interested in general in how weak laser pulses are useless [[SPS]] for QIP). | ||
+ | |||
+ | As well as those I did finally read: | ||
+ | |||
+ | # {{kurtsiefer00a}} Since 16:07 on {{thisday|31|December|2023}}. {{done|18:00 on {{thisday|31|December|2023}}}} |
From 31 December (2023) onward, I'm starting the new "tradition" of keeping track of the papers I need to read. By "read" I mean, really, "study" in some depth (skimming through a paper is the lot of the researcher).
As well as those I did finally read: