Reorientation-effect measurement of the 
〈21+∥Ê2∥21+〉
 matrix element in 
Ar36

Abstract Body effect is the key characteristic of DRAM cell transistor. Conventional method uses a TEG structure for body effect measurement. But this measurement is not accurate, because TEG structure has only several transistors and it is located outside of the DRAM die. This paper suggests a viable method for measuring DRAM cell transistor body effect. It uses a memory test system for fast, massive, nondestructive measurement. Newly developed method can measure 100,000 DRAM cell body effects in two minute, without sample damage. The test gives one median value and 100,000 individual values of body effects. Median value of measured body effects is equal to the TEG body effect. An individual DRAM cell body effect has a correlation with the fin height.

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Nonlinear effect measurement based on high‐speed optical transmission communication system

Microwave and Optical Technology Letters ◽

10.1002/mop.32207 ◽

2019 ◽

Vol 62 (4) ◽

pp. 1471-1476

Author(s):

Zhonghua Zhao ◽

Haiyan Xin ◽

Tao Liu

Keyword(s):

Communication System ◽

Nonlinear Effect ◽

High Speed ◽

Optical Transmission ◽

Effect Measurement

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Influence of nuclear thermometers and hot nuclei properties on nuclear temperature isospin effect measurement

Nuclear Physics A ◽

10.1016/j.nuclphysa.2021.122156 ◽

2021 ◽

Vol 1009 ◽

pp. 122156

Author(s):

Hui-Xiao Duan ◽

Dong-Hai Zhang ◽

Fan Zhang ◽

Hai-Shun Wu

Keyword(s):

Effect Measurement ◽

Hot Nuclei ◽

Nuclear Temperature

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K → μ+μ− as a clean probe of short-distance physics

Journal of High Energy Physics ◽

10.1007/jhep07(2021)103 ◽

2021 ◽

Vol 2021 (7) ◽

Author(s):

Avital Dery ◽

Mitrajyoti Ghosh ◽

Yuval Grossman ◽

Stefan Schacht

Keyword(s):

Matrix Element ◽

Standard Model ◽

Short Distance ◽

Time Dependent ◽

Final States ◽

Interference Effects ◽

Fundamental Theory ◽

Long Distance ◽

Ckm Matrix ◽

The Standard Model

Abstract The K → μ+μ− decay is often considered to be uninformative of fundamental theory parameters since the decay is polluted by long-distance hadronic effects. We demonstrate that, using very mild assumptions and utilizing time-dependent interference effects, ℬ(KS → μ+μ−)ℓ=0 can be experimentally determined without the need to separate the ℓ = 0 and ℓ = 1 final states. This quantity is very clean theoretically and can be used to test the Standard Model. In particular, it can be used to extract the CKM matrix element combination $$ \mid {V}_{ts}{V}_{td}\sin \left(\beta +{\beta}_s\right)\mid \approx \mid {A}^2{\lambda}^5\overline{\eta}\mid $$ ∣ V ts V td sin β + β s ∣ ≈ ∣ A 2 λ 5 η ¯ ∣ with hadronic uncertainties below 1%.

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