Methods and apparatuses for raman addressing of disjointed transition sets in D-manifold
Aspects of the present disclosure may include a method and/or a system for applying, to one or more ions in an ion chain, a first light beam having a first polarization and a second light beam having a second polarization to transfer the one or more ions from a first state of a first manifold to a second state of the first manifold, applying, to the one or more ions, the first light beam and the second light beam to transfer the one or more ions from the second state back to the first state, and applying, to the one or more ions, a third light beam to transition the one or more ions from the first state to a third state in a second manifold.
1 . A method of Raman addressing in a quantum information processing (QIP) system, comprising:
applying, to one or more ions in an ion chain, a first light beam having a first polarization and a second light beam having a second polarization to transfer the one or more ions from a first state of a first manifold to a second state of the first manifold, wherein the one or more ions in the first state includes a first angular momentum different than a second angular momentum in the second state;
applying, to the one or more ions, the first light beam and the second light beam to transfer the one or more ions from the second state back to the first state; and
applying, to the one or more ions, a third light beam to transition the one or more ions from the first state to a third state in a second manifold.
2 . The method of claim 1 , wherein applying the first light beam and the second light beam to transfer the one or more ions from the first state to the second state or from the second state to the first state comprises applying the first light beam in a co-propagating direction as the second light beam.
3 . The method of claim 1 , wherein the third beam is a global beam.
4 . The method of claim 1 , wherein the first light beam and the second light beam are circularly polarized light beams or elliptically polarized light beams.
5 . The method of claim 1 , further comprises applying a magnetic field parallel to the first light beam and the second light beam.
6 . The method of claim 1 , wherein the first light beam is σ + polarized and the second light beam is σ − polarized.
7 . The method of claim 1 , wherein applying the first light beam and the second light beam to transfer the one or more ions from the first state to the second state or from the second state to the first state comprises applying a single light beam having a first beat note associated with the first light beam and a second beat note associated with the second light beam.
8 . A non-transitory computer readable medium having instructions stored therein that, when executed by one or more processors of a quantum information processing (QIP) system, cause the one or more processors to:
control a first light source to apply, to one or more ions in an ion chain, a first light beam having a first polarization and a second light beam having a second polarization to transfer the one or more ions from a first state of a first manifold to a second state of the first manifold, wherein the one or more ions in the first state includes a first angular momentum different than a second angular momentum in the second state;
control the first light source to apply, to the one or more ions, the first light beam and the second light beam to transfer the one or more ions from the second state back to the first state; and
control a second light source to apply, to the one or more ions, a third light beam to transition the one or more ions from the first state to a third state in a second manifold.
9 . The non-transitory computer readable medium of claim 8 , wherein the instructions for applying the first light beam and the second light beam to transfer the one or more ions from the first state to the second state or from the second state to the first state comprises instructions for applying the first light beam in a co-propagating direction as the second light beam.
10 . The non-transitory computer readable medium of claim 8 , wherein the third beam is a global beam.
11 . The non-transitory computer readable medium of claim 8 , wherein the first light beam and the second light beam are circularly polarized light beams or elliptically polarized light beams.
12 . The non-transitory computer readable medium of claim 8 , further comprises instructions for controlling a magnetic system to apply a magnetic field parallel to the first light beam and the second light beam.
13 . The non-transitory computer readable medium of claim 8 , wherein the first light beam is σ + polarized and the second light beam is σ − polarized.
14 . The non-transitory computer readable medium of claim 8 , wherein the instructions for applying the first light beam and the second light beam to transfer the one or more ions from the first state to the second state or from the second state to the first state comprises instructions for applying a single light beam having a first beat note associated with the first light beam and a second beat note associated with the second light beam.
15 . A quantum information processing (QIP) system, comprising:
a first light source configured to:
apply, to one or more ions in an ion chain, a first light beam having a first polarization and a second light beam having a second polarization to transfer the one or more ions from a first state of a first manifold to a second state of the first manifold, wherein the one or more ions in the first state includes a first angular momentum different than a second angular momentum in the second state; and
apply, to the one or more ions, the first light beam and the second light beam to transfer the one or more ions from the second state back to the first state; and
a second light source configured to:
apply, to the one or more ions, a third light beam to transition the one or more ions from the first state to a third state in a second manifold.
16 . The QIP system of claim 15 , wherein applying the first light beam and the second light beam to transfer the one or more ions from the first state to the second state or from the second state to the first state comprises applying the first light beam in a co-propagating direction as the second light beam.
17 . The QIP system of claim 15 , wherein the third beam is a global beam.
18 . The QIP system of claim 15 , wherein the first light beam and the second light beam are circularly polarized light beams or elliptically polarized light beams.
19 . The QIP system of claim 15 , further comprises a magnetic system configured to apply a magnetic field parallel to the first light beam and the second light beam.
20 . The QIP system of claim 15 , wherein the first light beam is σ + polarized and the second light beam is σ − polarized.
21 . The QIP system of claim 15 , wherein applying the first light beam and the second light beam to transfer the one or more ions from the first state to the second state or from the second state to the first state comprises applying a single light beam having a first beat note associated with the first light beam and a second beat note associated with the second light beam.