Exercise 3.2

You Could Have Invented Monads! (And Maybe You Already Have.)

Show that lift f * lift g = lift (f.g)

——————————

The meaning of f' * g' should be (bind f') . (bind g') instead.

f' * g' = (bind f') . (bind g')
lift f = unit . f
f' = lift f

(lift f * lift g) (x, xs)
= (bind (lift f)) . (bind (lift g)) (x, xs)
= bind (lift f) (bind (lift g) (x, xs))
= bind (lift f) (gx, xs++gs)
  where
    (gx, gs) = (lift g) x

= bind (lift f) (gx, xs++gs)
  where
    (gx, gs) = (g x, "")

= bind (lift f) (g x, xs)

= (fx, xs++fs)
  where
    (fx, fs) = (lift f) gx
 
= (fx, xs++fs)
  where
    (fx, fs) = (f gx, "")

= (fx, xs)
  where
    (fx, fs) = (f (g x), "")

= (f (g x), xs)

bind f' (gx,gs) = (fx, gs++fs)
                  where
                    (fx,fs) = f' gx

bind (lift (f.g)) (x, xs)
= (hx, xs++hs)
  where
    (hx, hs) = (lift (f.g)) x

= (hx, xs++hs)
  where
    (hx, hs) = ((f.g) x, "")

= ((f (g x)), xs)

— Me@2015.07.19 11:04 PM

2015.10.02 Friday (c) All rights reserved by ACHK

Problem 14.3b1

A First Course in String Theory
 
 
14.3 Massive level in the open superstring.

~~~

What is the difference between “open bosonic string” and “open superstring”?

p.320 “With our conventions, these are world-sheet fermionic states that are now recognized to be states of spacetime fermions. The resulting, truncated sector is called the R- sector.”

NS(+): Equation (14.38) \left(\alpha' M^2 = 1, N^\perp = \frac{3}{2}\right):

\left\{ \alpha_{-1}^I b_{-1/2}^J, b_{-3/2}^I, b^I_{-1/2} b^J_{-1/2} b^K_{-1/2} \right\} | NS \rangle \otimes | p^+, \vec p_R \rangle

There are 128 states (cf. Quick Calculation 14.4).

R: Equation (14.54) \left(\alpha' M^2 = 1\right):

\alpha^I_{-1}  | R_a \rangle, d_{-1}^I | R_{\bar a} \rangle~||~\alpha^I_{-1}  | R_{\bar a} \rangle, d_{-1}^I | R_{a} \rangle

Only the left hand side represents the R- states.

Each of index I and index a has 8 possible values. So there are totally 64 states in the form of \alpha^I_{-1} | R_a \rangle.

Similarly, there are totally 64 states in the form of d_{-1}^I | R_{\bar a} \rangle.

Totally, for \alpha' M^2 = 1, there are 128 R- states.

— Me@2015-10-02 02:16:23 PM
 
 
 
2015.10.02 Friday (c) All rights reserved by ACHK