What are the units of probability density?











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Units of probability density? If bound electron is thought of as a cloud of charge, and it's charge density is proportional to the probability density. Then coulombs /m3 proportional to?










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    Units of probability density? If bound electron is thought of as a cloud of charge, and it's charge density is proportional to the probability density. Then coulombs /m3 proportional to?










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      Units of probability density? If bound electron is thought of as a cloud of charge, and it's charge density is proportional to the probability density. Then coulombs /m3 proportional to?










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      Units of probability density? If bound electron is thought of as a cloud of charge, and it's charge density is proportional to the probability density. Then coulombs /m3 proportional to?







      quantum-mechanics wavefunction units probability dimensional-analysis






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          The units of probability density in three-dimensional space are inverse volume, $[L]^{-3}$. This is because probability itself is a dimensionless number, such as 0.5 for a probability of 50%.



          A normalized wavefunction $Psi(vec{r},t)$ has dimensions $[L]^{-3/2}$ because the square of its complex magnitude, integrated over all space, must be 1. There is 100% probability that the electron is somewhere.



          The charge density at a point is the particle’s charge times the probability density at that point.



          When the wavefunction is for an electron, the charge density is $rho(vec{r},t)=-e|Psi(vec{r},t)|^2$, which could be expressed in units such as Coulombs per cubic meter ($text{C/m}^3$).






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            You can think about it by looking at what quantities you get from probability density. Namely, probability is dimensionless (it's just a number between 0 and 1), and given by the integral of probability density, so $P = int rho text{ d}V$.



            The volume element has dimensions $ [L]^3$, so the probability density must have dimensions $[L]^{-3}$.






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              2 Answers
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              The units of probability density in three-dimensional space are inverse volume, $[L]^{-3}$. This is because probability itself is a dimensionless number, such as 0.5 for a probability of 50%.



              A normalized wavefunction $Psi(vec{r},t)$ has dimensions $[L]^{-3/2}$ because the square of its complex magnitude, integrated over all space, must be 1. There is 100% probability that the electron is somewhere.



              The charge density at a point is the particle’s charge times the probability density at that point.



              When the wavefunction is for an electron, the charge density is $rho(vec{r},t)=-e|Psi(vec{r},t)|^2$, which could be expressed in units such as Coulombs per cubic meter ($text{C/m}^3$).






              share|cite|improve this answer



























                up vote
                6
                down vote













                The units of probability density in three-dimensional space are inverse volume, $[L]^{-3}$. This is because probability itself is a dimensionless number, such as 0.5 for a probability of 50%.



                A normalized wavefunction $Psi(vec{r},t)$ has dimensions $[L]^{-3/2}$ because the square of its complex magnitude, integrated over all space, must be 1. There is 100% probability that the electron is somewhere.



                The charge density at a point is the particle’s charge times the probability density at that point.



                When the wavefunction is for an electron, the charge density is $rho(vec{r},t)=-e|Psi(vec{r},t)|^2$, which could be expressed in units such as Coulombs per cubic meter ($text{C/m}^3$).






                share|cite|improve this answer

























                  up vote
                  6
                  down vote










                  up vote
                  6
                  down vote









                  The units of probability density in three-dimensional space are inverse volume, $[L]^{-3}$. This is because probability itself is a dimensionless number, such as 0.5 for a probability of 50%.



                  A normalized wavefunction $Psi(vec{r},t)$ has dimensions $[L]^{-3/2}$ because the square of its complex magnitude, integrated over all space, must be 1. There is 100% probability that the electron is somewhere.



                  The charge density at a point is the particle’s charge times the probability density at that point.



                  When the wavefunction is for an electron, the charge density is $rho(vec{r},t)=-e|Psi(vec{r},t)|^2$, which could be expressed in units such as Coulombs per cubic meter ($text{C/m}^3$).






                  share|cite|improve this answer














                  The units of probability density in three-dimensional space are inverse volume, $[L]^{-3}$. This is because probability itself is a dimensionless number, such as 0.5 for a probability of 50%.



                  A normalized wavefunction $Psi(vec{r},t)$ has dimensions $[L]^{-3/2}$ because the square of its complex magnitude, integrated over all space, must be 1. There is 100% probability that the electron is somewhere.



                  The charge density at a point is the particle’s charge times the probability density at that point.



                  When the wavefunction is for an electron, the charge density is $rho(vec{r},t)=-e|Psi(vec{r},t)|^2$, which could be expressed in units such as Coulombs per cubic meter ($text{C/m}^3$).







                  share|cite|improve this answer














                  share|cite|improve this answer



                  share|cite|improve this answer








                  edited yesterday

























                  answered yesterday









                  G. Smith

                  2,770615




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                      up vote
                      1
                      down vote













                      You can think about it by looking at what quantities you get from probability density. Namely, probability is dimensionless (it's just a number between 0 and 1), and given by the integral of probability density, so $P = int rho text{ d}V$.



                      The volume element has dimensions $ [L]^3$, so the probability density must have dimensions $[L]^{-3}$.






                      share|cite|improve this answer

























                        up vote
                        1
                        down vote













                        You can think about it by looking at what quantities you get from probability density. Namely, probability is dimensionless (it's just a number between 0 and 1), and given by the integral of probability density, so $P = int rho text{ d}V$.



                        The volume element has dimensions $ [L]^3$, so the probability density must have dimensions $[L]^{-3}$.






                        share|cite|improve this answer























                          up vote
                          1
                          down vote










                          up vote
                          1
                          down vote









                          You can think about it by looking at what quantities you get from probability density. Namely, probability is dimensionless (it's just a number between 0 and 1), and given by the integral of probability density, so $P = int rho text{ d}V$.



                          The volume element has dimensions $ [L]^3$, so the probability density must have dimensions $[L]^{-3}$.






                          share|cite|improve this answer












                          You can think about it by looking at what quantities you get from probability density. Namely, probability is dimensionless (it's just a number between 0 and 1), and given by the integral of probability density, so $P = int rho text{ d}V$.



                          The volume element has dimensions $ [L]^3$, so the probability density must have dimensions $[L]^{-3}$.







                          share|cite|improve this answer












                          share|cite|improve this answer



                          share|cite|improve this answer










                          answered 20 hours ago









                          Thomas Jones

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