Here is a little write-up of the deuteron problem — one of the possible problems on the Quantum II final last month. We show h
![Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration. - ppt download Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration. - ppt download](https://images.slideplayer.com/25/7870061/slides/slide_6.jpg)
Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration. - ppt download
![Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration. - ppt download Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration. - ppt download](https://images.slideplayer.com/25/7870061/slides/slide_10.jpg)
Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration. - ppt download
![Magnetic moment of neutrino and deuteron reaction T. Sato (Osaka U.) Motivation Neutrino disintegration of deuteron by electromagnetic interaction Summary. - ppt download Magnetic moment of neutrino and deuteron reaction T. Sato (Osaka U.) Motivation Neutrino disintegration of deuteron by electromagnetic interaction Summary. - ppt download](https://images.slideplayer.com/32/9997217/slides/slide_2.jpg)