Question about point mass prior and continuous distribution





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Suppose we have a point mass prior,



$$theta sim begin{cases} I(theta=1) ,& prob=frac{1}{2} \
Gamma(c,c), & prob=frac{1}{2} end{cases}$$



Then if we are asked



$lim_{c to infty} P(theta=1)$



Now here is the issue, since Gamma is a continuous distribution, it seems that in the case of gamma,we will never have $theta=1$.



To me it thus seems that regardless of the value of c, the $p(theta=1)=frac{1}{2}$



However, we also have that since expected value of a $gamma(a,b)=frac{a}{b}$ so that the expected value of the gamma is 1 when we have $a=b=c$



But, by Markov, for $X sim Gamma(c,c)$



$lim_{c to infty} Pr(|X-mu| lt epsilon) to 1$ for any $epsilon gt 0$



So is $lim_{c to infty}P(theta=1) =1$ , or is $lim_{c to infty}P(theta=1)=frac{1}{2}$



As even though the markov inequality holds, it is a continous distirbution, so we will never have it exactly equal to 1.



Thanks all










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    up vote
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    down vote

    favorite












    Suppose we have a point mass prior,



    $$theta sim begin{cases} I(theta=1) ,& prob=frac{1}{2} \
    Gamma(c,c), & prob=frac{1}{2} end{cases}$$



    Then if we are asked



    $lim_{c to infty} P(theta=1)$



    Now here is the issue, since Gamma is a continuous distribution, it seems that in the case of gamma,we will never have $theta=1$.



    To me it thus seems that regardless of the value of c, the $p(theta=1)=frac{1}{2}$



    However, we also have that since expected value of a $gamma(a,b)=frac{a}{b}$ so that the expected value of the gamma is 1 when we have $a=b=c$



    But, by Markov, for $X sim Gamma(c,c)$



    $lim_{c to infty} Pr(|X-mu| lt epsilon) to 1$ for any $epsilon gt 0$



    So is $lim_{c to infty}P(theta=1) =1$ , or is $lim_{c to infty}P(theta=1)=frac{1}{2}$



    As even though the markov inequality holds, it is a continous distirbution, so we will never have it exactly equal to 1.



    Thanks all










    share|cite|improve this question


























      up vote
      2
      down vote

      favorite









      up vote
      2
      down vote

      favorite











      Suppose we have a point mass prior,



      $$theta sim begin{cases} I(theta=1) ,& prob=frac{1}{2} \
      Gamma(c,c), & prob=frac{1}{2} end{cases}$$



      Then if we are asked



      $lim_{c to infty} P(theta=1)$



      Now here is the issue, since Gamma is a continuous distribution, it seems that in the case of gamma,we will never have $theta=1$.



      To me it thus seems that regardless of the value of c, the $p(theta=1)=frac{1}{2}$



      However, we also have that since expected value of a $gamma(a,b)=frac{a}{b}$ so that the expected value of the gamma is 1 when we have $a=b=c$



      But, by Markov, for $X sim Gamma(c,c)$



      $lim_{c to infty} Pr(|X-mu| lt epsilon) to 1$ for any $epsilon gt 0$



      So is $lim_{c to infty}P(theta=1) =1$ , or is $lim_{c to infty}P(theta=1)=frac{1}{2}$



      As even though the markov inequality holds, it is a continous distirbution, so we will never have it exactly equal to 1.



      Thanks all










      share|cite|improve this question















      Suppose we have a point mass prior,



      $$theta sim begin{cases} I(theta=1) ,& prob=frac{1}{2} \
      Gamma(c,c), & prob=frac{1}{2} end{cases}$$



      Then if we are asked



      $lim_{c to infty} P(theta=1)$



      Now here is the issue, since Gamma is a continuous distribution, it seems that in the case of gamma,we will never have $theta=1$.



      To me it thus seems that regardless of the value of c, the $p(theta=1)=frac{1}{2}$



      However, we also have that since expected value of a $gamma(a,b)=frac{a}{b}$ so that the expected value of the gamma is 1 when we have $a=b=c$



      But, by Markov, for $X sim Gamma(c,c)$



      $lim_{c to infty} Pr(|X-mu| lt epsilon) to 1$ for any $epsilon gt 0$



      So is $lim_{c to infty}P(theta=1) =1$ , or is $lim_{c to infty}P(theta=1)=frac{1}{2}$



      As even though the markov inequality holds, it is a continous distirbution, so we will never have it exactly equal to 1.



      Thanks all







      bayesian continuous-data






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      edited Nov 30 at 3:15

























      asked Nov 30 at 2:55









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          Your specified prior distribution is a mixture of a continuous and discrete part. Let $I sim text{Bern}(1/2)$ be the indicator that the parameter is taken from the gamma distribution. Then using the law of total probability you have:



          $$begin{equation} begin{aligned}
          mathbb{P}(theta = 1|c)
          &= mathbb{P}(theta = 1|c, I=0) cdot mathbb{P}(I=0) + mathbb{P}(theta = 1|c, I=1) cdot mathbb{P}(I=1) \[6pt]
          &= frac{1}{2} cdot mathbb{P}(theta = 1|c, I=0) + frac{1}{2} cdot mathbb{P}(theta = 1|c, I=1) \[6pt]
          &= frac{1}{2} + frac{1}{2} cdot mathbb{P}(theta = 1| theta sim text{Ga}(c,c)) \[6pt]
          &= frac{1}{2}. \[6pt]
          end{aligned} end{equation}$$



          (Note that the last step comes from recognising that the gamma is a continuous distribution, so the probability of a specific point is zero under this distribution.) This result holds for all values of $c$, so you are correct that it also holds in the limit:



          $$lim_{c rightarrow infty} mathbb{P}(theta = 1|c) = lim_{c rightarrow infty} frac{1}{2} = frac{1}{2}.$$



          Your later use of Chebychev's inequality shows that as $c rightarrow infty$ you get $theta rightarrow 1$ (convergence in probability), but this does not change the fact that $mathbb{P}(theta = 1|c) = 1/2$ for all $c > 0$. (To understand the reason for this more fully, have a read about the distinction between convergence in probability and almost-sure convergence.)






          share|cite|improve this answer





















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            1 Answer
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            1 Answer
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            up vote
            5
            down vote



            accepted










            Your specified prior distribution is a mixture of a continuous and discrete part. Let $I sim text{Bern}(1/2)$ be the indicator that the parameter is taken from the gamma distribution. Then using the law of total probability you have:



            $$begin{equation} begin{aligned}
            mathbb{P}(theta = 1|c)
            &= mathbb{P}(theta = 1|c, I=0) cdot mathbb{P}(I=0) + mathbb{P}(theta = 1|c, I=1) cdot mathbb{P}(I=1) \[6pt]
            &= frac{1}{2} cdot mathbb{P}(theta = 1|c, I=0) + frac{1}{2} cdot mathbb{P}(theta = 1|c, I=1) \[6pt]
            &= frac{1}{2} + frac{1}{2} cdot mathbb{P}(theta = 1| theta sim text{Ga}(c,c)) \[6pt]
            &= frac{1}{2}. \[6pt]
            end{aligned} end{equation}$$



            (Note that the last step comes from recognising that the gamma is a continuous distribution, so the probability of a specific point is zero under this distribution.) This result holds for all values of $c$, so you are correct that it also holds in the limit:



            $$lim_{c rightarrow infty} mathbb{P}(theta = 1|c) = lim_{c rightarrow infty} frac{1}{2} = frac{1}{2}.$$



            Your later use of Chebychev's inequality shows that as $c rightarrow infty$ you get $theta rightarrow 1$ (convergence in probability), but this does not change the fact that $mathbb{P}(theta = 1|c) = 1/2$ for all $c > 0$. (To understand the reason for this more fully, have a read about the distinction between convergence in probability and almost-sure convergence.)






            share|cite|improve this answer

























              up vote
              5
              down vote



              accepted










              Your specified prior distribution is a mixture of a continuous and discrete part. Let $I sim text{Bern}(1/2)$ be the indicator that the parameter is taken from the gamma distribution. Then using the law of total probability you have:



              $$begin{equation} begin{aligned}
              mathbb{P}(theta = 1|c)
              &= mathbb{P}(theta = 1|c, I=0) cdot mathbb{P}(I=0) + mathbb{P}(theta = 1|c, I=1) cdot mathbb{P}(I=1) \[6pt]
              &= frac{1}{2} cdot mathbb{P}(theta = 1|c, I=0) + frac{1}{2} cdot mathbb{P}(theta = 1|c, I=1) \[6pt]
              &= frac{1}{2} + frac{1}{2} cdot mathbb{P}(theta = 1| theta sim text{Ga}(c,c)) \[6pt]
              &= frac{1}{2}. \[6pt]
              end{aligned} end{equation}$$



              (Note that the last step comes from recognising that the gamma is a continuous distribution, so the probability of a specific point is zero under this distribution.) This result holds for all values of $c$, so you are correct that it also holds in the limit:



              $$lim_{c rightarrow infty} mathbb{P}(theta = 1|c) = lim_{c rightarrow infty} frac{1}{2} = frac{1}{2}.$$



              Your later use of Chebychev's inequality shows that as $c rightarrow infty$ you get $theta rightarrow 1$ (convergence in probability), but this does not change the fact that $mathbb{P}(theta = 1|c) = 1/2$ for all $c > 0$. (To understand the reason for this more fully, have a read about the distinction between convergence in probability and almost-sure convergence.)






              share|cite|improve this answer























                up vote
                5
                down vote



                accepted







                up vote
                5
                down vote



                accepted






                Your specified prior distribution is a mixture of a continuous and discrete part. Let $I sim text{Bern}(1/2)$ be the indicator that the parameter is taken from the gamma distribution. Then using the law of total probability you have:



                $$begin{equation} begin{aligned}
                mathbb{P}(theta = 1|c)
                &= mathbb{P}(theta = 1|c, I=0) cdot mathbb{P}(I=0) + mathbb{P}(theta = 1|c, I=1) cdot mathbb{P}(I=1) \[6pt]
                &= frac{1}{2} cdot mathbb{P}(theta = 1|c, I=0) + frac{1}{2} cdot mathbb{P}(theta = 1|c, I=1) \[6pt]
                &= frac{1}{2} + frac{1}{2} cdot mathbb{P}(theta = 1| theta sim text{Ga}(c,c)) \[6pt]
                &= frac{1}{2}. \[6pt]
                end{aligned} end{equation}$$



                (Note that the last step comes from recognising that the gamma is a continuous distribution, so the probability of a specific point is zero under this distribution.) This result holds for all values of $c$, so you are correct that it also holds in the limit:



                $$lim_{c rightarrow infty} mathbb{P}(theta = 1|c) = lim_{c rightarrow infty} frac{1}{2} = frac{1}{2}.$$



                Your later use of Chebychev's inequality shows that as $c rightarrow infty$ you get $theta rightarrow 1$ (convergence in probability), but this does not change the fact that $mathbb{P}(theta = 1|c) = 1/2$ for all $c > 0$. (To understand the reason for this more fully, have a read about the distinction between convergence in probability and almost-sure convergence.)






                share|cite|improve this answer












                Your specified prior distribution is a mixture of a continuous and discrete part. Let $I sim text{Bern}(1/2)$ be the indicator that the parameter is taken from the gamma distribution. Then using the law of total probability you have:



                $$begin{equation} begin{aligned}
                mathbb{P}(theta = 1|c)
                &= mathbb{P}(theta = 1|c, I=0) cdot mathbb{P}(I=0) + mathbb{P}(theta = 1|c, I=1) cdot mathbb{P}(I=1) \[6pt]
                &= frac{1}{2} cdot mathbb{P}(theta = 1|c, I=0) + frac{1}{2} cdot mathbb{P}(theta = 1|c, I=1) \[6pt]
                &= frac{1}{2} + frac{1}{2} cdot mathbb{P}(theta = 1| theta sim text{Ga}(c,c)) \[6pt]
                &= frac{1}{2}. \[6pt]
                end{aligned} end{equation}$$



                (Note that the last step comes from recognising that the gamma is a continuous distribution, so the probability of a specific point is zero under this distribution.) This result holds for all values of $c$, so you are correct that it also holds in the limit:



                $$lim_{c rightarrow infty} mathbb{P}(theta = 1|c) = lim_{c rightarrow infty} frac{1}{2} = frac{1}{2}.$$



                Your later use of Chebychev's inequality shows that as $c rightarrow infty$ you get $theta rightarrow 1$ (convergence in probability), but this does not change the fact that $mathbb{P}(theta = 1|c) = 1/2$ for all $c > 0$. (To understand the reason for this more fully, have a read about the distinction between convergence in probability and almost-sure convergence.)







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Nov 30 at 3:31









                Ben

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