Post on 20-Jan-2016
EXPERIMENTATION WITH BISMUTH SALTS SOLUTIONS
AND NEW IDEAS FOR CMNS EXPLANATION
D.S. Baranov, O.D. Baranova
Protvino Moscow region, Russiabaranovd@rambler.ru
Objectives
• Goal this job was the investigation of anomalous nuclear processes in the Bi salt experiment after strong electric field impact
• To explain results are attempt used the nuclear molecule model
• References• 1. D.S. Baranov, O.D. Baranova OBSERVATION
OF THE ISOMERS 212m1Bi AT THE EXPERIMENTS • WITH SOME BISMUTH SALTS AQUEOUS
SOLUTIONS International Conference Isomers in Nuclear and Interdisciplinary Research (INIR-2011)
• 2. . Baranov D.S., Baranova O.D. Production of Neutron-rich Bi Isotopes by Electric Fields. INTERNATIONAL SYMPOSIUM ON EXOTIC NUCLEI (EXON2009). AIP CONFERENCE PROCEEDINGS VOLUME 1224 P 241-246 http://proceedings.aip.org/proceedings
Sample preparation
Experimental set up
Counts in detector №1
0 30 60 90 120 150 180 2100
5
10
15
20
25
30
35
40
45co
un
ts
time (mins)
exp fity0 2 ±0A1 53.17731 ±7.13849t1 59.01378 ±11.09016
nitrate bismuth alpha activity
0 30 60 90 120 150 180 210
0
5
10
15
20
25
30
35
40
Ядро Периодыполураспада
Брен.%
Схемы распадов МэВ
γ-излучение(МэВ)
Деф.м,е кэВ
207Bi 38 лет Э. З. β+ 0,57(98), 1,77 -20058208Bi 3,68·10 5 лет Э. З. 2,614 -18879209Bi 2·1019 лет 100 → α (4,88 ) 205Pb -18268210Bi 5,013 сут ~100 β (1,16 )210Po→α (5,35 ) 206Pb 0,803(0,0011) -14738210Bim1 3·106 лет 99,6 → α (5 ) 206Tl 0,34, 0,61… 271,3e
211Bi 2,14 мин 99,7 → α (6,62) 207Tl 0,351(14) -11865212Bi 60,6мин;2,98·10-6с 64
36 β (2,25 )212Po →α (8,78) 208Pb → α (6,05) 208Tl
0,727(7), 1,62(1,8)…
-8135
212Bim1
25 мин; 2,98·10-6с 33 67
β (2,25)212Po→ α (8,78 ) 208Pb → α (6,05 ) 208Tl
250e
212Bim2 7 мин; 45,1 с 100 β(1,95)212Pom→α(11,68 )208Pb 2200e
213Bi 45,6мин; 4,2·10-6с 97,8 β (1,39) 213Po α (8,38) 209Pb 0,437 -5247214Bi 19,9мин;1,64·10-4с ~100 β (3,26) 214Po α (7,69) 210Pb 0,6(47)… -1209215Bi 7,7мин;1,78·10-3с ~100 β () 215Po → α (7,38 ) 211Pb 1710215Bim1 36,4мин;1,78·10-3с ~100 β () 215Po → α (7,38 ) 211Pb 1347e
216Bi 3,6мин; 0,15с ~100 β () 216Po → α (6,78 ) 212Pb 5970c217Bi 98.5 c; < 10с ~100 β () 217Po → α (6,55 ) 213Pb218Bi 33 с; 3,05 мин ~100 β (5.06 ) 218Po →α (6,0) 214Pb
Scheme of 212Bi decay
Event example
Detector 1 Experiment data 05.10.2007
Photo 18.10.2007 M= 7 : 1 Photo 05.05.2009 Alpha count 10.3+-0.6 Alpha count 17.2+-1.1
Bi isotopes production for 7.5 hours in a closed Si detecto 4 on pieces of bismuth nitrate, made by
the cumulative emissions
dN/dE for alpha
after 70 mins count in the first 70 mins
Alpha to beta time delay
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
10
20
30
40
Model: ExpDec1 Chi^2 = 0.15816R^2 = 0.98811 y0 0 ±0A1 46.82147 ±9.95447t1 0.36571 ±0.06108
cou
nts
time delay (mcsec)
beta + alpha delayd events
0 2 4 6 8 10 12 14 16 18 20
0
10
20
30
40
dN/dE for electrons
0,0 0,5 1,0 1,5 2,0 2,50
4
8
12
16
20
24
experiment data theor. data /7/
cou
nts
electron energy (MeV)
0,0 0,5 1,0 1,5 2,0 2,5
0
4
8
12
16
20
24
• We detected 210Bi, 212Bi, 212m1Bi, 214Bi.
• Bismuth 211 and 213 were not found.
• Such scheme of decay is impossible for free nucleus. Thus we need to introduce the system of nucleare
Nuclear molecules Atom Vigier
size 100 Fermi
Traces on Si detector surfaceline – Nuclear molecule position
Silicium plate edge near the woll
Crater
Микроскоп фирмы АМФОРА 80*80 мкм
Energy deposition 0.0001 G
Дет.2
Craters
Project:BaranovOwner: INCA OperatorElevation= 35.0 deg. Tilt= 0.0 deg. Azimuth= 0.0 deg.Sample: 19-05-2011Type: DefaultSample is polished and coated with Carbon - thickness (nm): 15.0, density (g/cm3): 2.25.Thresholding has been selected : All quantitative results below 0 sigma have been set to zero.Site: Sample-1 Spectrum: Spectrum 1 19-май-2011 02:05 PMEnergy Resn. Area TOT.AR. L./R.time(s) P.time U(kV) Perr. .0 49.15 273789 83154 70.00/89.41 6 20.00 95.45%Counted by INCAINCA Proc.Option: Oxygen by stoichiometryElmt A.C.% IntC. Wt% 2*Swt% At% Comp% dComp% FormulaS K 6.57 1.0763 6.10 0.50 15.81 15.24 1.25 SO3 5.46Bi M 34.51 0.9324 37.01 2.18 14.71 41.26 2.43 Bi2O3 5.08O 13.38 0.96 69.48 24.00Total 56.50+/- 2.43 CompSum 56.50+/- 2.73 CatSum 10.54 An.Sum 24.00
Site: Sample-2Spectrum: Spectrum 1 19-май-2011 02:38 PMEnergy Resn. Area TOT.AR. L./R.time(s) P.time U(kV) Perr. .0 49.15 273789 111140 100.00/126.33 6 20.00 95.45%Peak omited: 0.800 keVCounted by INCA/Oxygen by stoichiometryINCA Proc.Option: All elements analyzedElmt A.C.% IntC. Wt% 2*Swt% At% Comp% dComp% FormulaN K 5.24 1.2944 4.05 1.96 19.89 15.62 7.56 N2O5 7.14O K 10.06 0.6471 15.54 1.30 66.84 -0.66 < 7.85 O 24.00Bi M 37.10 0.9201 40.32 1.52 13.27 44.95 1.69 Bi2O3 4.76Total 59.91+/- 2.80 CompSum 60.57+/- 7.74 CatSum 11.91 An.Sum 24.00
11C 40.48O 5.63Si 52.80K 0.35
Au 0.74
12C 37.38O 4.32Si 57.13K 0.29
Au 0.87
13C 91.28O 1.20Si 6.91K 0.25Ca 0.12Au 0.24
14C 58.66O 26.87Si 13.62Na 0.34Ca 0.28Au 0.23
15
Si 100.00
16C 17.43O 2.72Si 78.61
Au 1.24
10C 16.91
Si 81.62
Au 1.46
11C 48.91O 3.69Si 39.18N 7.62Au 0.60
12C 37.02O 2.42Si 59.72
Au 0.84
13C 33.85O 3.79Si 60.76K 0.65Au 0.95
14C 20.97O 9.01Si 67.16K 1.67Au 1.20
“Snake” traces
2C 49.63O 31.54Si 5.85Al 2.85 Zn 5.91Bi 4.22
3C 42.44O 9.27Si 45.88Ca 0.13Zn 0.74Br 0.21Au 0.71Bi 0.64
4C 62.19O 14.94Si 18.89Al 0.59 Zn 1.89Au 0.47Bi 1.03
5C 20.44Si 78.26Au 1.30
6C 28.14Si 70.76Au 1.10
7C 51.55O 20.41Al 0.78Si 23.30Zn 2.29Au 0.58Bi 1.09
8C 55.66O 28.16Al 1.63Si 6.03Ca 0.23Cu 0.43Zn 4.86Bi 3.01
9C 58.40O 28.07Al 1.21Si 1.40Zn 4.17Bi 6.74
Tail
Head10C 47.75O 39.67Al 2.03Si 0.44Zn 4.66Cu 0.77Bi 4.67
9C 55.53O 20.97Al 0.80Si 18.04Zn 2.06Au 0.61Bi 1.99
8C 63.79O 12.59Al 0.24Si 21.62Zn 0.77Au 0.49Bi 0.50
1.We have evidens that giant long-lived nuclear molecules were detected in the experiments with bismuth salts solution.
2. We suppous that nuclear molecules are the part of every CMNS prosess.
3. We need to continue our investigations
Conclusion
Thank you
1 Russan CF Conf.
1993 г. Moscow-Blaсk See train