Abstract: Described is a method comprising directing an ultra-low voltage electron beam to a surface of a first insulating layer. The first insulating layer is disposed on a second insulating layer. The method includes modifying, by the application of the ultra-low voltage electron beam, the surface of the first insulating layer to selectively switch an interface between a first state having a first electronic property and a second state having a second electronic property.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: Described is a method comprising directing an ultra-low voltage electron beam to a surface of a first insulating layer. The first insulating layer is disposed on a second insulating layer. The method includes modifying, by the application of the ultra-low voltage electron beam, the surface of the first insulating layer to selectively switch an interface between a first state having a first electronic property and a second state having a second electronic property.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second. layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: A structure includes an electronically controllable ferromagnetic oxide structure that includes at least three layers. The first layer comprises STO. The second layer has a thickness of at least about 3 unit cells, said thickness being in a direction substantially perpendicular to the interface between the first and second layers. The third layer is in contact with either the first layer or the second layer or both, and is capable of altering the charge carrier density at the interface between the first layer and the second layer. The interface between the first and second layers is capable of exhibiting electronically controlled ferromagnetism.

Abstract: A reconfigurable device includes a first insulating layer, a second insulating layer, and a nanoscale quasi one- or zero-dimensional electron gas region disposed at an interface between the first and second insulating layers. The device is reconfigurable by applying an external electrical field to the electron gas, thereby changing the conductivity of the electron gas region. A method for forming and erasing nanoscale-conducting structures employs tools, such as the tip of a conducting atomic force microscope (AFM), to form local electric fields. The method allows both isolated and continuous conducting features to be formed with a length well below 5 nm.

Abstract: A reconfigurable device and a method of creating, erasing, or reconfiguring the device are provided. At an interface between a first insulating layer and a second insulating layer, an electrically conductive, quasi one- or zero-dimensional electron gas is present such that the interface presents an electrically conductive region that is non-volatile. The second insulating layer is of a thickness to allow metal-insulator transitions upon the application of a first external electric field. The electrically conductive region is subject to erasing upon application of a second external electric field.

Abstract: A reconfigurable device and a method of creating, erasing, or reconfiguring the device are provided. At an interface between a first insulating layer and a second insulating layer, an electrically conductive, quasi one- or zero-dimensional electron gas is present such that the interface presents an electrically conductive region that is non-volatile. The second insulating layer is of a thickness to allow metal-insulator transitions upon the application of a first external electric field. The electrically conductive region is subject to erasing upon application of a second external electric field.

Abstract: A reconfigurable device includes a first insulating layer, a second insulating layer, and a nanoscale quasi one- or zero-dimensional electron gas region disposed at an interface between the first and second insulating layers. The device is reconfigurable by applying an external electrical field to the electron gas, thereby changing the conductivity of the electron gas region. A method for forming and erasing nanoscale-conducting structures employs tools, such as the tip of a conducting atomic force microscope (AFM), to form local electric fields. The method allows both isolated and continuous conducting features to be formed with a length well below 5 nm.

Abstract: A reconfigurable device and a method of creating, erasing, or reconfiguring the device are provided. At an interface between a first insulating layer and a second insulating layer, an electrically conductive, quasi one- or zero-dimensional electron gas is present such that the interface presents an electrically conductive region that is non-volatile. The second insulating layer is of a thickness to allow metal-insulator transitions upon the application of a first external electric field. The electrically conductive region is subject to erasing upon application of a second external electric field.

Abstract: A reconfigurable device and a method of creating, erasing, or reconfiguring the device are provided. At an interface between a first insulating layer and a second insulating layer, an electrically conductive, quasi one- or zero-dimensional electron gas is present such that the interface presents an electrically conductive region that is non-volatile. The second insulating layer is of a thickness to allow metal-insulator transitions upon the application of a first external electric field. The electrically conductive region is subject to erasing upon application of a second external electric field.

Abstract: A nanoscale device and a method for creating and erasing of nanoscale conducting regions at the interface between two insulating oxides SrTiO3 and LaAlO3 is provided. The method uses the tip of a conducting atomic force microscope to locally and reversibly switch between conducting and insulating states. This allows ultra-high density patterning of quasi zero or one dimensional electron gas conductive regions, such as nanowires and conducting quantum dots respectively. The patterned structures are stable at room temperature after removal of the external electric field.

Abstract: A nanoscale device and a method for creating and erasing of nanoscale conducting regions at the interface between two insulating oxides SrTiO3 and LaAlO3 is provided. The method uses the tip of a conducting atomic force microscope to locally and reversibly switch between conducting and insulating states. This allows ultra-high density patterning of quasi zero or one dimensional electron gas conductive regions, such as nanowires and conducting quantum dots respectively. The patterned structures are stable at room temperature after removal of the external electric field.

Abstract: The development of a multiple-channel dual phase lock-in optical spectrometer (LIOS) is presented, which enables parallel phase-sensitive detection at the output of an optical spectrometer. The light intensity from a spectrally broad source is modulated at the reference frequency, and focused into a high-resolution imaging spectrometer. The height at which the light enters the spectrometer is controlled by an acousto-optic deflector, and the height information is preserved at the output focal plane. A two-dimensional InGaAs focal plane array collects light that has been dispersed in wavelength along the horizontal direction, and in time along the vertical direction. The data is demodulated using a high performance computer-based digital signal processor. This parallel approach greatly enhances (by more than 100×) the speed at which spectrally resolved lock-in data can be acquired.

Abstract: The development of a multiple-channel dual phase lock-in optical spectrometer (LIOS) is presented, which enables parallel phase-sensitive detection at the output of an optical spectrometer. The light intensity from a spectrally broad source is modulated at the reference frequency, and focused into a high-resolution imaging spectrometer. The height at which the light enters the spectrometer is controlled by an acousto-optic deflector, and the height information is preserved at the output focal plane. A two-dimensional InGaAs focal plane array collects light that has been dispersed in wavelength along the horizontal direction, and in time along the vertical direction. The data is demodulated using a high performance computer-based digital signal processor. This parallel approach greatly enhances (by more than 100×) the speed at which spectrally resolved lock-in data can be acquired.