Quantum bit reading device and method
An apparatus includes a material in a resonator and containing systems, each of the systems having five energy states, a unit generating first and second pulse that resonate in a second transition and a third transition, respectively, a unit controlling the first and second pulse to make the first and second pulse temporally overlap each other to obtain third light, a unit emitting the third light to each system, a unit generating observation light to be coupled to the resonator mode, a unit introducing the observation light to the resonator from an outside thereof, a unit reading one of quantum bits by measuring an intensity of one of reflected light and transmitted light of the observation light, a unit controlling the first and second pulse to make the first and second pulse temporally overlap each other to obtain fourth light, and a unit emitting the fourth light to each system.
1. A quantum bit reading apparatus comprising:
a resonator having a resonator mode;
a material included in the resonator and containing n physical systems (n is an integer not less than 2), each of the physical systems having at least five energy states, a first transition of each physical system between |g> i and |e 1 > i resonating in the resonator mode, and |0> i and |1> i representing quantum bits, where the five energy states of each physical system i (i is a natural number not more than n) are expressed by |0> i , |1> i , |g> i , |e 1 > i and |e 2 > i in increasing order of energy;
a first generation unit configured to generate first pulse light and second pulse light that resonate in a second transition between |g> i and |e 2 > i and a third transition between |1> i and |e 2 > i , respectively;
a first control unit configured to control the first pulse light and the second pulse light to make the first pulse light and the second pulse light temporally overlap each other to obtain third light formed of the first pulse light and the second pulse light, a state of the third light being shifted from a first state in which a first intensity of the first pulse light is higher than a second intensity of the second pulse light, to a second state in which the second intensity is higher than the first intensity;
a first emission unit configured to emit the third light to each physical system i;
a second generation unit configured to generate observation light to be coupled to the resonator mode;
an introducing unit configured to introduce the observation light to the resonator from an outside thereof;
a reading unit configured to read one of the quantum bits by measuring a third intensity of at least one of reflected light of the observation light and transmitted light of the observation light;
a second control unit configured to control, after the one quantum bit is read, the first pulse light and the second pulse light to make the first pulse light and the second pulse light temporally overlap each other to obtain fourth light formed of the first pulse light and the second pulse light, a state of the fourth light being shifted from the second state to the first state; and
a second emission unit configured to emit the fourth light to each physical system i.
2. The apparatus according to claim 1 , wherein when measuring the third intensity, the reading unit adjusts a time T m of the measuring to satisfy T g <T m <T e , T g being an inverse number of twice a coupling constant between the resonator mode and each physical system, or T g =1/(2×g), T e being a lifetime of an excited state |e 1 > of each physical system.
3. The apparatus according to claim 1 , further comprising a cryostat which holds an interior thereof at a constant temperature, wherein the resonator and the material are included in the cryostat.
4. A quantum bit reading apparatus comprising:
a resonator having a resonator mode;
a material included in the resonator and containing n physical systems (n is an integer not less than 2), each of the physical systems having at least five energy states, a first transition of each physical system between |g> i and |e 1 > i resonating in the resonator mode, and |0> i and |1> i representing quantum bits, where the five energy states of each physical system i (i is a natural number not more than n) are expressed by |0> i , |1> i , |g> i , |e 1 > i and |e 2 > i in increasing order of energy;
a first generation unit configured to generate first pulse light and second pulse light that resonate in a second transition between |g> i and |e 2 > i and a third transition between |1> i and |e 2 > i , respectively;
a control unit configured to control the first pulse light and the second pulse light to make the first pulse light and the second pulse light temporally overlap each other to obtain third light formed of the first pulse light and the second pulse light, a state of the third light being shifted from a first state in which a first intensity of the first pulse light is higher than a second intensity of the second pulse light, to a second state in which the second intensity is higher than the first intensity;
a first emission unit configured to emit the third light to each physical system i;
a second generation unit configured to generate observation light to be coupled to the resonator mode;
an introducing unit configured to introduce the observation light to the resonator from an outside thereof;
a reading unit configured to read one of the quantum bits by measuring a third intensity of at least one of reflected light of the observation light and transmitted light of the observation light; and
a second emission unit configured to emit, to each physical system i, light that resonates in one of the first transition and the second transition, after the one quantum bit is read.
5. The apparatus according to claim 4 , wherein when measuring the third intensity, the reading unit adjusts a time T m of the measuring to satisfy T g <T m <T e , T g being an inverse number of twice a coupling constant between the resonator mode and each physical system, or T g =1/(2×g), T e being a duration of an excited state |e 1 > of each physical system.
6. The apparatus according to claim 4 , further comprising a cryostat which holds an interior thereof at a constant temperature, wherein the resonator and the material are included in the cryostat.
7. A quantum bit reading method comprising:
preparing a resonator having a resonator mode;
preparing a material included in the resonator and containing n physical systems (n is an integer not less than 2), each of the physical systems having at least five energy states, a first transition of each physical system between |g> i and |e 1 > i resonating in the resonator mode, and |0> i and |1> i representing quantum bits, where the five energy states of each physical system i (i is a natural number not more than n) are expressed by |0> i , |1> i , |g> i , |e 1 > i and |e 2 > i in increasing order of energy;
generating first pulse light and second pulse light that resonate in a second transition between |g> i and |e 2 > i and a third transition between |1> i and |e 2 > i , respectively;
controlling the first pulse light and the second pulse light to make the first pulse light and the second pulse light temporally overlap each other to obtain third light formed of the first pulse light and the second pulse light, a state of the third light being shifted from a first state in which a first intensity of the first pulse light is higher than a second intensity of the second pulse light, to a second state in which the second intensity is higher than the first intensity;
emitting the third light to each physical system i;
generating observation light to be coupled to the resonator mode;
introducing the observation light to the resonator from an outside thereof;
reading one of the quantum bits by measuring a third intensity of at least one of reflected light of the observation light and transmitted light of the observation light;
controlling, after the one quantum bit is read, the first pulse light and the second pulse light to make the first pulse light and the second pulse light temporally overlap each other to obtain fourth light formed of the first pulse light and the second pulse light, a state of the fourth light being shifted from the second state to the first state; and
emitting the fourth light to each physical system i.
8. The method according to claim 7 , wherein when measuring the third intensity, a time T m of the measuring is adjusted to satisfy T g <T m <T e , T g being an inverse number of twice a coupling constant between the resonator mode and each physical system, or T g =1/(2×g), T e being a duration of an excited state |e 1 > of each physical system.
9. The method according to claim 7 , further comprising preparing a cryostat which holds an interior thereof at a constant temperature, wherein the resonator and the material are included in the cryostat.
10. A quantum bit reading method comprising:
preparing a resonator having a resonator mode;
preparing a material included in the resonator and containing n physical systems (n is an integer not less than 2), each of the physical systems having at least five energy states, a first transition of each physical system between |g> i and |e 1 > i resonating in the resonator mode, and |0> i and |1> i representing quantum bits, where the five energy states of each physical system i (i is a natural number not more than n) are expressed by |0> i , |1> i , |g> i , |e 1 > i and |e 2 > i in increasing order of energy;
generating first pulse light and second pulse light that resonate in a second transition between |g> i and |e 2 > i and a third transition between |1> i and |e 2 > i , respectively;
controlling the first pulse light and the second pulse light to make the first pulse light and the second pulse light temporally overlap each other to obtain third light formed of the first pulse light and the second pulse light, a state of the third light being shifted from a first state in which a first intensity of the first pulse light is higher than a second intensity of the second pulse light, to a second state in which the second intensity is higher than the first intensity;
emitting the third light to each physical system i;
generating observation light to be coupled to the resonator mode;
introducing the observation light to the resonator from an outside thereof;
reading one of the quantum bits by measuring a third intensity of at least one of reflected light of the observation light and transmitted light of the observation light; and
emitting, to each physical system i, light that resonates in one of the first transition and the second transition, after the one quantum bit is read.
11. The method according to claim 10 , wherein when measuring the third intensity, a time T m of the measuring is adjusted to satisfy T g <T m <T e , T g being an inverse number of twice a coupling constant between the resonator mode and each physical system, or T g =1/(2×g), T e being a duration of an excited state |e 1 >of each physical system.
12. The method according to claim 10 , further comprising preparing a cryostat which holds an interior thereof at a constant temperature, wherein the resonator the material are included in the cryostat.