beta minus造句

• The primary mode for the heavier isotopes is beta minus ( & beta;  " ) decay.
• However, explanations of beta minus decay always gives this outcome & ndash; is there a reason why?
• The primary decay mode for isotopes lighter than 153 Eu is electron capture, and the primary mode for heavier isotopes is beta minus decay.
• The primary decay modes before the most abundant stable isotope, 142 Nd, are electron capture and positron decay, and the primary mode after is beta minus decay.
• If beta minus decay occurs by a down quark changing into an up quark by the emission of a talk ) 13 : 34, 7 September 2008 ( UTC)
• After this radiative capture, Th-232 becomes Th-233, which undergoes two beta minus decays resulting in the production of the fissile isotope U-233.
• Since uranium is present in MOX, although plutonium will be burnt, second generation plutonium will be produced through the radiative capture of U-238 and the two subsequent beta minus decays.
• Th-232 is a fertile material that can undergo a neutron capture reaction and two beta minus decays, resulting in the production of fissile activity curve of the SNF around 1 million years.
• Using beta minus decay ) that yields a new nucleus ( the emitter nucleus ) in an excited state that emits an additional neutron, called a " delayed " neutron, to get to ground state.
• Positron emission should not be confused with electron emission or beta minus decay ( ?  " decay ), which occurs when a neutron turns into a proton and the nucleus emits an electron and an antineutrino.
• Th-232 is a fertile material that can undergo a neutron capture reaction and two beta minus decays, resulting in the production of fissile activity curve of the SNF around 1, 000, 000 years.
• The indium isotopes lighter than 115 In predominantly decay through electron capture or positron emission to form cadmium isotopes, while the other indium isotopes from 115 In and greater predominantly decay through beta minus decay to form tin isotopes.
• For example, during beta minus decay, a down quark within a neutron is changed into an up quark, thus converting the neutron to a proton and resulting in the emission of an electron and an electron antineutrino.
• A few lighter particles may be created or destroyed ( example : beta minus and beta plus decay, or electron capture decay ), but these minor processes are not important to the immediate energy release in fission and fusion.
• A proton can change into a neutron by emitting a positron ( beta plus ), and a neutron can change into a proton by emitting an electron ( beta minus ) .  Keenan Pepper 03 : 59, 1 December 2005 ( UTC)
• My read of the chart in that article is that the method of day is not super important; that's just a reflection of whatever kind of instability there is ( beta minus happens when you're on the left side of the " stable " line; beta plus when you're on the right, alpha if you're too far up and to the right, etc . ).