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SUMMARY

The forum discussion focuses on the analysis of beta decay patterns in uranium isotopes using the NUDAT database, which reveals a double peak curve in decay rates. The conversation also touches on the potential correlation between the availability of excited states in nuclei and the observed decay peaks. Additionally, participants inquire about the historical detection of a massive charged scalar boson by L3 and OPAL experiments, referencing specific papers and the implications for nuclear decay processes.

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  • Understanding of beta decay and its significance in nuclear physics.
  • Familiarity with the NUDAT database for nuclear data analysis.
  • Knowledge of the concepts of phase space in nuclear decay processes.
  • Awareness of high-energy physics and previous findings related to scalar bosons.
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  • Research the NUDAT database for detailed beta decay data and trends.
  • Explore the implications of excited nuclear states on decay processes.
  • Investigate the historical context and findings of L3 and OPAL experiments regarding scalar bosons.
  • Study the concept of nuclear driplines and their relevance to particle physics.
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Researchers in nuclear physics, high-energy physicists, and anyone interested in the intricacies of beta decay and particle detection in experimental physics.

arivero
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Time ago I went to the NUDAT database to plot the number of known beta decays for each mass number; this is expected to reproduce the double peak curve of uranium decay, because of course more research have been done in the subproducts of this decay and then more excited, beta decaying, states are known. But I wonder if it could be argued in the contrary way: than the uranium decays into these peaks because the nuclei in the area have more excited states available, thus more phase space to decay into.

Attached you can see the plot first as as a curve/density plot in the (Z,N) plane, and as a histogram in the mass number A=Z+N.
 

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arivero said:
Time ago I went to the NUDAT database to plot the number of known beta decays for each mass number; this is expected to reproduce the double peak curve of uranium decay, because of course more research have been done in the subproducts of this decay and then more excited, beta decaying, states are known. But I wonder if it could be argued in the contrary way: than the uranium decays into these peaks because the nuclei in the area have more excited states available, thus more phase space to decay into.

Attached you can see the plot first as as a curve/density plot in the (Z,N) plane, and as a histogram in the mass number A=Z+N.

Hi Alex,

Tell me, when did L3 and OPAL see a massive charged scalar boson in that range? I saw this note in the histogram, around 70 or 75 GeV, and I was wondering because I had not heard of one since the unconfirmed LEP find in 2001 (which was at much higher mass anyway, closer to 100 GeV). Furthurmore, does the amplitude of beta decay die off near or around the start of the alpha decay dripline? I am not so much into atomic/nuclear physics as I am into nuclear/high-energy physics, so I am not quite as familiar with this, but I do remember your past paper on the nuclear dripline coincidences regarding boson masses. That was quite a few years ago.

Regards,
Patrick
 
mormonator_rm said:
Hi Alex,

Tell me, when did L3 and OPAL see a massive charged scalar boson in that range?
let me check: it is somewhere here

hep-ex/9909044, hep-ex/0009010, hep-ex/0105057

specially in the later. Thus before the 115 one. It took a good bunck of remix and analysis to clear it out, and yet it causes a small hole in the plots for 95% confidence level.

And yep, you have got good memory, I mentioned it in my puzzle of the driplines. Lubos argued against, on very reasonable theoretical grounds, I think to remember. But anyway, I was just reporting data. Amusing data.
 
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