Final answer:
To construct an NPDA that accepts language (a) L = {a"b²n: n>0}, we can use a stack to keep track of the number of b's. The NPDA can start by pushing a marker symbol onto the stack and transitions based on the input. for hence, option (b) is the correct answer.
Step-by-step explanation:
To construct an NPDA that accepts language (a) L = {a"b²n: n>0}, we can use a stack to keep track of the number of b's. The NPDA can start by pushing a marker symbol onto the stack. Then, for each 'a' input, it pops nothing from the stack and transitions to the next state. For each 'b' input, it pops a single 'b' from the stack. If the stack is empty after processing all inputs, the NPDA accepts the input string.
In particle physics, reactions must adhere to conservation laws, such as the conservation of strangeness, which is violated in reaction (b) p+n→p+p+K¯. For antiparticle decays, a muon antiparticle (μ+) decays into a positron and an electron neutrino (μ+ → e+ + ve), which conserves lepton number.
The student's question involves particle physics reactions and the conservation laws that govern these reactions. Specifically, the conservation of strangeness is crucial in understanding which particle reactions can occur. The question asks which of the following reactions cannot occur because they violate the law of conservation of strangeness. The law of conservation of strangeness states that the strangeness of a system must remain constant in any process that occurs via the strong interaction. However, changes in strangeness can occur through weak interactions which proceed more slowly than strong interactions.
Given the reactions provided, we can tell that the reaction (b) p+n→p+p+K¯ would violate the law of conservation of strangeness because antikaons, K¯, have strangeness +1 while protons and neutrons have no strangeness. This means the final state has a different total strangeness than the initial state, which violates the law when considering that the process is a strong interaction.
Regarding decay processes for antiparticles, for a muon antiparticle (μ+), one possible decay is μ+ → e+ + ve. This decay process conserves lepton number, as a muon lepton changes into an electron lepton, and the corresponding neutrinos account for the rest of the lepton balance.