 | |
 |
 |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
 | |
|
 |
|
 |
 | |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
|
 |
Researching QTM Properties with the QTS Toolkit
Make the Interferometer Oscillating
Introduce more 
marker states to produce oscillating interferometer graphs. For example, define a new QTM state q1 as
q1 = InitQTM[2,b,Interval[{-4,8}],{{-3,b[1]},{-1,b[1]},{1,b[1]},{3,b[1]},{5,b[1]},{7,b[1]}},9,h,-3]
in formatted form:
Rerun the step operator and compare with the previous results.
Check if T is Orthogonality Preserving
Provide numerical evidence, that T is orthogonality preserving (i.e., 
. For a strict mathematical proof, see [17].
Setup the adjoint step operator as TCADJ and performSameQ[FmtState[TC[TCADJ[u]], FmtState[TCADJ[TC[u]]]]] for u=Nest[TC,qc,n] and large n values.
Check if T is Distinct Path Generating
Provide numerical evidence that T is distinct path generating. For a strict mathematical proof, see [17].
Solution:
Show that QInner[u,TC[u]]=0.
Use u=Nest[TC,qc,n] for large n.
Do the same for TADJ.
Copyright © 2002 Wolfram Media, Inc. All rights reserved.