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4Semester
IQC
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Cards (25)
Every Qubit is in
superposition
between
0 or 1
A variable x can be in
superposition
between
all values
Any probalistic process can be written as
nxn-matrix
A
Pr[output j | input i]
=
A_ji
Probabilistic -> Quantum :
distributions ->
quantum state
probabilities ->
amplitudes
deterministic possibilities ->
classical possibilities/states
processes
(stoch. matrices) ->
unitary matrices
Probabilistically -> Quantumly
distribution is a
vector
because it "mixes"
deterministic possabilities
->
quantum state is a
vector
because
superposition
"mixes"
classical possabilities
Quantum systems
are described by a list of n classical
possibilities
A quantum state is a vector
ψ
∈
C
n
\psi \in \mathbb{C}^n
ψ
∈
C
n
with
∑
∣
ψ
i
∣
2
=
\sum |\psi_i|^2 =
∑
∣
ψ
i
∣
2
=
1
1
1
or
∣
∣
ψ
∣
∣
=
||\psi|| =
∣∣
ψ
∣∣
=
1
1
1
Valid quantum processes are
unitary matrices
A (square) matrix U is
unitary
if
∣
∣
U
ψ
∣
∣
=
||U_\psi||=
∣∣
U
ψ
∣∣
=
1
1
1
when
∣
∣
ψ
∣
∣
=
||\psi||=
∣∣
ψ
∣∣
=
1
1
1
U is
unitary
if
U
t
U
=
U^t U =
U
t
U
=
I
−
>
(
U
t
=
k
o
n
j
u
g
i
e
r
t
+
t
r
a
n
s
p
o
n
i
e
r
t
)
I -> (U^t = konjugiert + transponiert)
I
−
>
(
U
t
=
k
o
nj
ug
i
er
t
+
t
r
an
s
p
o
ni
er
t
)
Description of Systems
List of deterministic possibilities 1,...,N ->
Probabilistic
List of
classical
possibilities 1,...,N ->
Quantum
State of Systems
N-vector
ψ
∈
R
n
=
\psi \in \mathbb{R}^n =
ψ
∈
R
n
=
probabilistic distribution
∑
ψ
i
=
\sum \psi_i =
∑
ψ
i
=
1
,
ψ
i
>
=
1, \psi_i >=
1
,
ψ
i
>=
0
0
0
N-vector
ψ
∈
C
n
=
\psi \in \mathbb{C}^n =
ψ
∈
C
n
=
quantum state
∑
∣
ψ
i
∣
2
=
\sum |\psi_i|^2 =
∑
∣
ψ
i
∣
2
=
1
1
1
Development of system
Probabilistic:
Stochastic
matrix
∈
R
N
x
N
\in R^{NxN}
∈
R
N
x
N
(Every column is
probabilistic
distribution)
Quantum
Unitary
matrix
U
U
∈
C
N
x
N
U\in \mathbb{C}^{NxN}
U
∈
C
N
x
N
maps
quantum
state to
quantum state
U
t
U
=
U^t U =
U
t
U
=
I
I
I
Given
distribution
μ
\mu
μ
, if we observe it , get outcome i with
prob
μ
i
\mu_i
μ
i
and in that : new distribution is :
e
i
e_i
e
i
:= (0,...,0,1,0,...0) at the i-th element
Measurments do change the system
Observation : Probabilitic -> Quantum
Update of
knowledge
->
State becomes
e_i
-> physical effect -> no superposition -> no
interference
∣∣ϕ∣∣= sqrt(
∑
\sum
∑
|
ϕ
i
\phi_i
ϕ
i
|^2)
Hadamard
H
=
1
2
\frac 1 {\sqrt2}
2
1
(
1
1
1
−
1
\begin{matrix} 1&1\\1&-1 \end{matrix}
1
1
1
−
1
)
You are given a n-dimensional probability distribution vector x.What is the average (a.k.a.
mean value
) of the entries x_i? :
1/n
A quantum measurement changes the outcome probabilities of
future observations.
Consider a vector x∈R^n and a vector y∈R^m. Then the tensor product x⊗y is in R^k.
The value of k is
n*m
|
+
> :=
1
2
\frac 1 {\sqrt2}
2
1
|0> +
1
2
\frac 1 {\sqrt2}
2
1
|1> = H(|
0
>)
|
-
> :=
1
2
\frac 1 {\sqrt2}
2
1
|0> -
1
2
\frac 1 {\sqrt2}
2
1
|1> = H(|
1
>)
H(|+>)
= H(
1
2
∣
0
>
\frac 1 {\sqrt2}|0>
2
1
∣0
>
+
1
2
∣
1
>
\frac 1 {\sqrt2}|1>
2
1
∣1
>
) = 1/2(|
0
> + |
1
>) + 1/2(|
0
> - |
1
>) = |
0
>
H(
|->) = H(
1
2
∣
0
>
\frac 1 {\sqrt2}|0>
2
1
∣0
>
-
1
2
∣
1
>
\frac 1 {\sqrt2}|1>
2
1
∣1
>
) = 1/2(|0> + |1>) - 1/2(|0> - |1>) = |1>