Metric for 2D de Sitter?












3












$begingroup$


What is the correct metric to use for two dimensional de Sitter? If one starts with the following metric, which looks similar to de Sitter in 4 dimensions:



$$ds^2 = -dt^2 + e^{2H t} dx^2,$$



one can calculate $R = 2H^2$, and $R_{00} = -H^2$, which gives the $Lambda = 0$, which is not the solution one is looking for. What should be the correct metric to use for the same?










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$endgroup$

















    3












    $begingroup$


    What is the correct metric to use for two dimensional de Sitter? If one starts with the following metric, which looks similar to de Sitter in 4 dimensions:



    $$ds^2 = -dt^2 + e^{2H t} dx^2,$$



    one can calculate $R = 2H^2$, and $R_{00} = -H^2$, which gives the $Lambda = 0$, which is not the solution one is looking for. What should be the correct metric to use for the same?










    share|cite|improve this question











    $endgroup$















      3












      3








      3


      2



      $begingroup$


      What is the correct metric to use for two dimensional de Sitter? If one starts with the following metric, which looks similar to de Sitter in 4 dimensions:



      $$ds^2 = -dt^2 + e^{2H t} dx^2,$$



      one can calculate $R = 2H^2$, and $R_{00} = -H^2$, which gives the $Lambda = 0$, which is not the solution one is looking for. What should be the correct metric to use for the same?










      share|cite|improve this question











      $endgroup$




      What is the correct metric to use for two dimensional de Sitter? If one starts with the following metric, which looks similar to de Sitter in 4 dimensions:



      $$ds^2 = -dt^2 + e^{2H t} dx^2,$$



      one can calculate $R = 2H^2$, and $R_{00} = -H^2$, which gives the $Lambda = 0$, which is not the solution one is looking for. What should be the correct metric to use for the same?







      general-relativity differential-geometry metric-tensor de-sitter-spacetime






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      edited Dec 10 '18 at 5:46









      Qmechanic

      103k121851177




      103k121851177










      asked Dec 10 '18 at 1:59









      Michael WilliamsMichael Williams

      11810




      11810






















          1 Answer
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          $begingroup$

          In two-dimensional spacetime, the Einstein tensor $R_{ab}-frac{1}{2}g_{ab}R$ is identically zero , which explains why you get $Lambda=0$.



          In any number $D$ of spacetime dimensions, including $D=2$, de Sitter spacetime can be constructed like this. Start with the $D+1$ dimensional Minkowski metric
          $$
          -(mathrm dX^0)^2+sum_{k=1}^D(mathrm dX^k)^2.
          tag{1}
          $$

          The submanifold defined by the condition
          $$
          sum_{k=1}^D(X^k)^2=L^2+(X^0)^2
          tag{2}
          $$

          is $D$-dimensional de Sitter spacetime. The length parameter $L$ is related to the cosmological constant $Lambda$ by
          $$
          Lambda = frac{(D-2)(D-1)}{2L^2}.
          tag{3}
          $$

          This is equation (4) in "Les Houches Lectures on de Sitter Space". Setting $D=2$ recovers your result $Lambda=0$.



          By the way, equations (13)-(14) in the same paper show how to derive the de Sitter metric in the form
          $$
          -mathrm dt^2+e^{2t}sum_{k=1}^{D-1}(mathrm dx^k)^2
          $$

          starting from equations (1)-(2). For $D=2$, this reduces to the form shown in the question.






          share|cite|improve this answer











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            1 Answer
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            active

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            5












            $begingroup$

            In two-dimensional spacetime, the Einstein tensor $R_{ab}-frac{1}{2}g_{ab}R$ is identically zero , which explains why you get $Lambda=0$.



            In any number $D$ of spacetime dimensions, including $D=2$, de Sitter spacetime can be constructed like this. Start with the $D+1$ dimensional Minkowski metric
            $$
            -(mathrm dX^0)^2+sum_{k=1}^D(mathrm dX^k)^2.
            tag{1}
            $$

            The submanifold defined by the condition
            $$
            sum_{k=1}^D(X^k)^2=L^2+(X^0)^2
            tag{2}
            $$

            is $D$-dimensional de Sitter spacetime. The length parameter $L$ is related to the cosmological constant $Lambda$ by
            $$
            Lambda = frac{(D-2)(D-1)}{2L^2}.
            tag{3}
            $$

            This is equation (4) in "Les Houches Lectures on de Sitter Space". Setting $D=2$ recovers your result $Lambda=0$.



            By the way, equations (13)-(14) in the same paper show how to derive the de Sitter metric in the form
            $$
            -mathrm dt^2+e^{2t}sum_{k=1}^{D-1}(mathrm dx^k)^2
            $$

            starting from equations (1)-(2). For $D=2$, this reduces to the form shown in the question.






            share|cite|improve this answer











            $endgroup$


















              5












              $begingroup$

              In two-dimensional spacetime, the Einstein tensor $R_{ab}-frac{1}{2}g_{ab}R$ is identically zero , which explains why you get $Lambda=0$.



              In any number $D$ of spacetime dimensions, including $D=2$, de Sitter spacetime can be constructed like this. Start with the $D+1$ dimensional Minkowski metric
              $$
              -(mathrm dX^0)^2+sum_{k=1}^D(mathrm dX^k)^2.
              tag{1}
              $$

              The submanifold defined by the condition
              $$
              sum_{k=1}^D(X^k)^2=L^2+(X^0)^2
              tag{2}
              $$

              is $D$-dimensional de Sitter spacetime. The length parameter $L$ is related to the cosmological constant $Lambda$ by
              $$
              Lambda = frac{(D-2)(D-1)}{2L^2}.
              tag{3}
              $$

              This is equation (4) in "Les Houches Lectures on de Sitter Space". Setting $D=2$ recovers your result $Lambda=0$.



              By the way, equations (13)-(14) in the same paper show how to derive the de Sitter metric in the form
              $$
              -mathrm dt^2+e^{2t}sum_{k=1}^{D-1}(mathrm dx^k)^2
              $$

              starting from equations (1)-(2). For $D=2$, this reduces to the form shown in the question.






              share|cite|improve this answer











              $endgroup$
















                5












                5








                5





                $begingroup$

                In two-dimensional spacetime, the Einstein tensor $R_{ab}-frac{1}{2}g_{ab}R$ is identically zero , which explains why you get $Lambda=0$.



                In any number $D$ of spacetime dimensions, including $D=2$, de Sitter spacetime can be constructed like this. Start with the $D+1$ dimensional Minkowski metric
                $$
                -(mathrm dX^0)^2+sum_{k=1}^D(mathrm dX^k)^2.
                tag{1}
                $$

                The submanifold defined by the condition
                $$
                sum_{k=1}^D(X^k)^2=L^2+(X^0)^2
                tag{2}
                $$

                is $D$-dimensional de Sitter spacetime. The length parameter $L$ is related to the cosmological constant $Lambda$ by
                $$
                Lambda = frac{(D-2)(D-1)}{2L^2}.
                tag{3}
                $$

                This is equation (4) in "Les Houches Lectures on de Sitter Space". Setting $D=2$ recovers your result $Lambda=0$.



                By the way, equations (13)-(14) in the same paper show how to derive the de Sitter metric in the form
                $$
                -mathrm dt^2+e^{2t}sum_{k=1}^{D-1}(mathrm dx^k)^2
                $$

                starting from equations (1)-(2). For $D=2$, this reduces to the form shown in the question.






                share|cite|improve this answer











                $endgroup$



                In two-dimensional spacetime, the Einstein tensor $R_{ab}-frac{1}{2}g_{ab}R$ is identically zero , which explains why you get $Lambda=0$.



                In any number $D$ of spacetime dimensions, including $D=2$, de Sitter spacetime can be constructed like this. Start with the $D+1$ dimensional Minkowski metric
                $$
                -(mathrm dX^0)^2+sum_{k=1}^D(mathrm dX^k)^2.
                tag{1}
                $$

                The submanifold defined by the condition
                $$
                sum_{k=1}^D(X^k)^2=L^2+(X^0)^2
                tag{2}
                $$

                is $D$-dimensional de Sitter spacetime. The length parameter $L$ is related to the cosmological constant $Lambda$ by
                $$
                Lambda = frac{(D-2)(D-1)}{2L^2}.
                tag{3}
                $$

                This is equation (4) in "Les Houches Lectures on de Sitter Space". Setting $D=2$ recovers your result $Lambda=0$.



                By the way, equations (13)-(14) in the same paper show how to derive the de Sitter metric in the form
                $$
                -mathrm dt^2+e^{2t}sum_{k=1}^{D-1}(mathrm dx^k)^2
                $$

                starting from equations (1)-(2). For $D=2$, this reduces to the form shown in the question.







                share|cite|improve this answer














                share|cite|improve this answer



                share|cite|improve this answer








                edited Dec 10 '18 at 8:25









                Lorenzo B.

                1765




                1765










                answered Dec 10 '18 at 3:53









                Dan YandDan Yand

                9,20611536




                9,20611536






























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