In nuclear reaction `._2He^4 ._zX^A rarr._(z + 2) Y^(A + 3) + A`, denotes.

In nuclear reaction ._(4)Be^(4)+._(z)X^(A)rarr._(z+2)Y^(A+3)+R , R denotes

In nuclear reaction ""_(2)He^(4) + ""_(z)X^(A) to ""_(z+2)Y^(A+3) +A , denotes

In the nuclear reaction ._85 X^297 rarr Y + 4 alpha, Y is.

In nuclear reaction "" _(2) He ^(4)+ "" _(z) X ^(A) to "" _(z+2) Y ^(A+3) + R R denotes

In the nuclear reaction ._92 U^238 rarr ._z Th^A + ._2He^4 , the values of A and Z are.

In nuclear reaction ._(4)Be^(9)+._(2)He^(4)rarr._(6)C^(12)+X,X will be

A nuclear reaction given by 1_Z X^A rarr .(Z+1) Y^A + ._(-1)e^0 + vecp represents.

The particles emitted in the nuclear reaction are respectively - ._(Z)X^(A) rarr ._(Z + A)Y^(A) rarr._(Z - 1)R^(A - 4) rarr._(Z - 1)R^(A - 4)

Balance the following nuclear reactions: a. ._(3)Li^(7) + ._(0)n^(1) rarr 2 ._(2)He^(4) + ? b. ._(42)Mo^(94) + ._(1)H^(2) rarr ._(0)n^(1) + ?

Consider the follwing nuclear reactions: ._(92)^(238) M rarr ._(y)^(x)N + 2 ._(2)He^(4) ._(y)^(x)N rarr ._(B)^(A)L + 2beta^(+)