The low-energy limit of the four-point 3-loop amplitude (including its overall coefficient) is computed in both type IIA and IIB superstring theories using the pure spinor formalism. The result is shown to agree with the prediction of the coefficient for the type IIB $D^6 R^4$ interaction made by Green and Vanhove based on S-duality considerations
The full two-loop amplitudes for five massless states in Type II and Heterotic superstrings are cons...
The full two-loop amplitudes for five massless states in Type~II and Heterotic superstrings are cons...
We compute explicitly the four-particle amplitude in superstring theories by using the hyperelliptic...
The low-energy limit of the massless two-loop five-point amplitudes for both type IIA and type IIB s...
Explicit expressions for one-loop five supergraviton scattering amplitudes in both type II superstri...
Explicit expressions for one-loop five supergraviton scattering amplitudes in both type II superstri...
The low-energy limit of the massless two-loop five-point amplitudes for both type IIA and type IIB s...
In an earlier paper, we constructed the genus-two amplitudes for five external massless states in Ty...
Explicit expressions for one-loop five supergraviton scattering amplitudes in both type II superstri...
This thesis discusses how the pure spinor formalism can be used to efficiently compute superstring s...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
The pure spinor formalism for the superstring has recently been used to compute massless four-point ...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
The full two-loop amplitudes for five massless states in Type II and Heterotic superstrings are cons...
The full two-loop amplitudes for five massless states in Type~II and Heterotic superstrings are cons...
We compute explicitly the four-particle amplitude in superstring theories by using the hyperelliptic...
The low-energy limit of the massless two-loop five-point amplitudes for both type IIA and type IIB s...
Explicit expressions for one-loop five supergraviton scattering amplitudes in both type II superstri...
Explicit expressions for one-loop five supergraviton scattering amplitudes in both type II superstri...
The low-energy limit of the massless two-loop five-point amplitudes for both type IIA and type IIB s...
In an earlier paper, we constructed the genus-two amplitudes for five external massless states in Ty...
Explicit expressions for one-loop five supergraviton scattering amplitudes in both type II superstri...
This thesis discusses how the pure spinor formalism can be used to efficiently compute superstring s...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
The pure spinor formalism for the superstring has recently been used to compute massless four-point ...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
Using the results recently obtained for computing integrals over (non-minimal) pure spinor superspac...
The full two-loop amplitudes for five massless states in Type II and Heterotic superstrings are cons...
The full two-loop amplitudes for five massless states in Type~II and Heterotic superstrings are cons...
We compute explicitly the four-particle amplitude in superstring theories by using the hyperelliptic...
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