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Try-catch makes the code tidy and readable, without try-catch the code becomes ugly as you need to check the result and handle exceptions after each function call. However, it is performed in run-time and have overhead each time a function is called?
Add/remove code usually changes the execution speed of the program. Which could affects the timing between different tasks, such as timeout mechanism or time restrictions in real-time systems. In the extreme case, the execution could be blocked and causes starvations/deadlocks. Add/remove code actually affects the program counter.
It should be helpful to prevent deadlock by checking each statement one by one in the locked area and make sure each one will not block the execution.
svnadmin cteate /tmp/tstprj
mkdir /tmp/workdir
cd /tmp/workdir
svn co file:///tmp/tstprj
cd tstprj
cp /etc/fstab .
svn add fstab
svn ci --username=justin
cat << 'EOF' > /tmp/PrintPos.sh
#!/bin/bash
c=$#
i=1
while [ $i -le $c ]; do
echo "\$$i='$1'"
shift
i=$(($i + 1))
done
EOF
chmod a+x /tmp/PrintPos.sh
cat << 'EOF' > /tmp/ConcurDiffWrap.sh
#!/bin/bash
## !! There is interval between @a1@ and @a2@ such that other process would
## interfere the execution within the interval.
NewTmpDir()
{
local Node
while :; do
Node=$RANDOM
if [ ! -e /tmp/${Node} ]; then # @a1@
mkdir /tmp/${Node} # @a2@
eval "${1}=/tmp/${Node}"
return
fi
done
}
NewTmpDir Dir
mv "$6" "${Dir}/Old" || echo 'Cannot move $6'
echo '' > "$6"
mv "$7" "${Dir}/New" || echo 'Cannot move $7'
echo '' > "$7"
meld "$1" "$2" "$3" "$4" "$5" "${Dir}/Old" "${Dir}/New" &
## Print positional parameters.
##
## Put this segment at positions where positional parameter are no longer used,
## becasue there are `shift' in this segment.
c=$#
i=1
while [ $i -le $c ]; do
echo "\$$i='$1'"
shift
i=$(($i + 1))
done
echo '==================================================================='
EOF
chmod a+x /tmp/ConcurDiffWrap.sh
svn di -r 2:3 --diff-cmd /tmp/ConcurDiffWrap.sh
"Any quantum circuit can be simulated to an arbitrary degree of accuracy using a combination of CNOT gates and single qubit rotations." - Controlled NOT gate
"Because the number of elements in the matrices is , where x is the number of qubits the gates act on, it is intractable to simulate large quantum systems using classical computers." - Quantum_gate#Circuit_composition_and_entangled_states
For example, state means that the first qubit is 0 and the second qubit is 1. If, for example, , it means that state appears with probability 0.7 after measurements.
The above map is the result of a series of quntum program executions which applying CNOT gate on the system. But you can not know the map beforehand, so how to know the value of the second qubit after applying the quantum gate operation above? Here is what you may do:
You should be able to encode the system so that each state appears with the probability according to your design. Suppose that you encode the system so that the probability distribution is
(note that )
Suppose that you want to know the second qubit's value of state after the quantum operation. Because the corresponding probability you have encoded is , you should be able to find one of 4 after-operation states , , and appears with probability 0.2 as you repeat the quantum program over and over several times. And you will finally realize that state appears with probability 0.2 after you repeat enough the quantum program, so it means the state transition is from to and therefore the second qubit's value changes from 0 to 1 after the quantum operation.
Adiabatic quantum computation
BKL singularity
BadVista
Bing
Bing (Search)
Bing (search engine)
Bing (web search engine)
Cavity quantum electrodynamics
Classical test theory
Cluster state
Coherence (physics)
Convolution
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Criticism of Windows 7
Device driver
Dirac delta function
Direct Rendering Manager
Euler's theorem (differential geometry)
Evolute
Fourier series
Freedesktop.org
Git (software)
Google
Google platform
Graphics Execution Manager
Guievict
Internet Explorer 8
Jordan curve theorem
Keith Packard
LOCC
Lagrange's identity
Library (computing)
List of unsolved problems in physics
Loadable kernel module
MeeGo
MeeGo (operating system)
Method of characteristics
Metric tensor
MicroXwin
Microsoft
Microsoft Office 2007
Möbius transformation
Nitrogen-vacancy center
O(1) scheduler
Office Open XML
One-way quantum computer
OpenDocument
OpenDocument software
Optical lattice
Optical pumping
Overlap-add method
Overlap–add method
Phasor
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Pseudo-differential operator
Pythagorean triple
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Quantum channel
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Quantum error correction
Quantum gate
Quantum information
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Quantum mechanical Bell test prediction
Quantum programming
Quantum teleportation
Quasiconformal mapping
Qubit
Ratio test
Riesz transform
Selection rule
Separable state
Separable states
Squashed entanglement
Standardization of Office Open XML
Sturm-Liouville theory
Sturm–Liouville theory
Superconducting quantum computing
Topological computing
Topological quantum computer
Trapped ion quantum computer
Universal quantum simulator
Unsolved problems in physics
Wayland (display server)
Wayland (display server protocol)
Wayland display server
Windowing system
Windows 7
Windows 7/Archive 7
X Window System
Xmove
Xpra
User:HAl
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