Erratum to “Characterization of low-energy nuclear reactions involving emission of few non-relativistic particles” [Nucl. Instr. and Meth. A 622 (2010) 642–649]

Erratum to “Characterization of low-energy nuclear reactions involving emission of few non-relativistic particles” [Nucl. Instr. and Meth. A 622 (2010) 642–649]

Nuclear Instruments and Methods in Physics Research A 694 (2012) 313 Contents lists available at SciVerse ScienceDirect Nuclear Instruments and Meth...

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Nuclear Instruments and Methods in Physics Research A 694 (2012) 313

Contents lists available at SciVerse ScienceDirect

Nuclear Instruments and Methods in Physics Research A journal homepage: www.elsevier.com/locate/nima

Erratum

Erratum to ‘‘Characterization of low-energy nuclear reactions involving emission of few non-relativistic particles’’ [Nucl. Instr. and Meth. A 622 (2010) 642–649] D. Martinez Heimann a,b,n, A.J. Pacheco a,b, O.A. Capurro a a b

´n Nacional de Energı´a Ato ´mica, Av. Gral. Paz 1499, B1650KNA San Martı´n, Argentina Departamento de Fı´sica, Laboratorio TANDAR, Comisio CONICET, Av. Rivadavia 1917, C1033AAJ Buenos Aires, Argentina

The publisher regrets for the below errors in a few equations. The asymptotic directions of emission in Eq. (2) should have been indicated as vectors in boldface. The corresponding line should read:

X111112 , X1112 , X12 , and

ð2Þ

Some equations in the Appendix are affected by incorrect notation (scalars instead of vectors in (A1); missing operator symbols for scalar product in (A2)–(A5); missing operator symbols for vector product in (A4) and (A5)), missing factors in the left-hand side of (A4) and (A5), and wrong indices and a missing term in the second line of (A7). These errors do not affect any other section of the original article. The correct expressions are the following: Vjð1Þ ¼ Vjð1Þ Xj or Vjð2Þ ¼ Vjð2Þ Xj , Tj ¼ 0  5

2 X

mi VjðiÞ  VjðiÞ ,

with j ¼ 122,1112,111112,. . .

i ¼ 1,2

ðA1Þ

ðA2Þ

i¼1

Vjð1Þ Vj1ð1Þ cosðyj Þ ¼ Vjð1Þ  Vj1ð1Þ

ðA3Þ

 2     Vjð1Þ Vj1ð1Þ  Vj2ð1Þ sinyj1 sinyj cosfj ¼ Vj2ð1Þ  Vj1ð1Þ  Vjð1Þ  Vj1ð1Þ

ðA4Þ

 3     Vjð1Þ Vj1ð1Þ  Vj2ð1Þ sinyj1 sinyj sinfj ¼ Vj2ð1Þ  Vj1ð1Þ  Vjð1Þ  Vj1ð1Þ  Vj1ð1Þ

ðA5Þ

uK ð1Þ ¼ Vcm þ

K X

Vjð1Þ

ðA7Þ

j ¼ 12

uLð2Þ ¼ Vcm þ

L1 X

Vjð1Þ þVLð2Þ

for L ¼ 122 to K

j ¼ 12

Also, in accordance with the modification of the second line of (A7), the final sentence of the Appendix should be replaced by: ‘‘where K represents the last binary plane and L indicates any plane (from 1–2 to K)’’.

n

DOI of original article: http://dx.doi.org/10.1016/j.nima.2010.07.063 Corresponding author at: Departamento de Fı´sica, Laboratorio TANDAR, Comisio´n Nacional de Energı´a Ato´mica, Av. Gral. Paz 1499, B1650KNA San Martı´n, Argentina. E-mail address: [email protected] (D. Martinez Heimann).

0168-9002/$ - see front matter & 2012 Elsevier B.V. All rights reserved. http://dx.doi.org/10.1016/j.nima.2012.08.054