STELLAR NUCLEOSYNTHESIS OF ELEMENTS HIGHER THAN ATOMIC NUMBER 30, (NI)

 

 

By:Clarence L. Dulaney

      2226 Fairgreen Drive

       Missouri City, TX 77489

        cldtx1@sbcglobal.net  

 

 

 

A: INTRODUCTION

 

It is pretty well established that stellar energy is produced by fusion reactions forming elements up to atomic number 30, (Ni).  [1, 2, 3, 4].  No further energy or fusion occurs for elements above 30Ni.[4.320]  (Note:  4 is the reference number and 320 is the page number).

 

That higher elements than 30Ni are produced even in the sun is indicated by Novotony’s [1.47ff] “Table of Abundances” based on spectral data from sunspots and the solar photosphere.  Obviously some mechanism must exist to produce these higher elements (up to 92U). 

 

B,  Addition of “Neutrons” to Heavy Elements

 

The current theory has addition of “neutrons” in a step-by-step fashion to form the higher isotopes.  Clayton [2.Chapter 7] gives a detailed account of the process, although he is a bit vague about where the “neutrons” come from particularly in stars as light as the sun.  He is also vague about how the heavy nuclei and “neutrons” come in contact.  (this, along with some comments about what “neutrons” actually are will be addressed in a subsequent paper.)

 

“Neutrons” can add with essentially no energy because they have no charge.  They are not accelerated to high velocities in the high temperature of the stellar atmospheres.   They are added to a given atomic number up to the point where an unstable nucleus is formed.  Then a B- is emitted and the next higher atomic number element is produced.   The neutron capture is “slow” with the  b- emission being relatively fast.  The overall process is called the “s-process”. 

 

 30Ni62 + 0n1 = 30Ni63*  = 31Cu63 =b-.      31Cu63 +0n1  = 31Cu64      etc.  is an example of the process.

 

As evidence for the s-process, spectral lines of 43Tc and 61Pr have been found in spectra from “s-type” red-giant stars[5].  Both of these elements have no ”stable” isotopes and are not found naturally on earth or in the solar abundances.

 

Pathways ro produce most stable isotopes of the heavy elements have been shown to be possible [2]   There are some isotopes however that cannot be reached by the s-process.  See Lilley, [4.332] for evidence that there is a problem  with 40Zr96 and with 42Mo100.  Other problems concern “stable” isotopes of 90Th and 92U.

 

Theory has it that these isotopes are made by the “r-process”, so named for the rapid addition of a large number of “neutrons” that leads to bypassing possible unstable nuclei.  Generally, only in nova type explosions are enough “neutrons” available for the  r-process “ to occur.  With the large number of “neutrons”, the addition proceeds to transuranic isotopes.  These isotopes spontaneously undergo fission.  As an example, 97Bk could disintegrate to 48Cd and 49In.

 

Nowever,  Novotny’s Table show that some of the r-process elements show up in the solar atmosphere, so the process must stop before transuranic isotopes are formed, (or very large number of :neutrons” are produced on the sun.)   This topic will also be addressed in the next paper. 

 

There is one other possible process called the “p-process” that produces isotopes with higher ratios of protons to neutrons than the 

 

s- or r-processes.  Actually it should be called the g-process.[6].

See the next paper.

 

 

SUMMARY

 

 

No energy is produced (other than a small “binding” energy) in addition of “neutrons’ to elements higher than 30Ni in stellar atmospheres. 

 

Current theory has it that higher atomic weight isotopes are formed by addition of “neutrons” one-by-one,  Once an unstable isotope is formed, the next higher atomic number isotope is formed by b- decay.

 

Two pathways are proposed, the “s-process” and the “r-process”.  The former involves slow addition of “neutrons” followed by fast emission of b-..

 

The “r-process” involves rapid addition of large number of “neutrons” which skips over some unstable nuclei.

 

By one  process or the other all stable isotopes up to 92U are formed.

 

 

REFERENCES

 

 

1.    e. Novotony, “Introduction to Stellar Atmospheres and Interiors”, Oxford University Press, NY, 1973

2.    D. D. Clayton, “Principles of Stellar Evolution and Nucleosynthesis”,  McGraw-Hill, NY, 1968

3.    J. M. Paschakoff, “Astronomy, From the Earth to the Universe,”, Saunders College Press, Philadelphia, 1977

4.    J. Lilley, “Nuclear Physics, Principles and Applications” John Wiley &Sons, NY, 2001

5.    www.Wikipedia/Technetium

6.    www.Wikipedia/p-process

 

 

© September 14, 2007   Clarence L. Dulaney