2.
    发明专利
    未知

    公开(公告)号:DE68917310T2

    公开(公告)日:1995-03-09

    申请号:DE68917310

    申请日:1989-12-13

    Applicant: IBM

    Abstract: The Delta-Phi microlens consists of a first foil (3) of a metal or alloy from the group of transition metals and a second foil (4) of a metal or alloy from the group comprising the elements of IA or IIA groups of the periodic system of elements, the second foil (4) being coated onto one surface of said first foil (3). A hole (2) extends through both foils (3, 4) in precise alignment with the axis (6) of a sharply pointed tip (1) made of conductive material and placed at a distance of the order of 1 mu m from that surface of said first foil (3) opposite said second foil (4). With the first foil (3) connected to ground and a potential on the order of -30 V applied at said tip (1), at ultra-high vacuum conditions, a beam of low-energy electrons will have trajectories (5) deviated towards a focal point (7). With a positive potential of more than 30 V applied to said tip (1), and in a noble gas atmosphere, a beam of ions passing through the microlens of the invention will have trajectories (5) deflected towards said focal point (7).

    3.
    发明专利
    未知

    公开(公告)号:DE3887891T2

    公开(公告)日:1994-08-11

    申请号:DE3887891

    申请日:1988-11-01

    Applicant: IBM

    Abstract: This source for charged particles comprises a sharply pointed tip (1) and an aperture (2) in a thin sheet of material. If the point of the tip (1) is made sharp enough, i.e., if it ends in a single atom or a trimer of atoms, the electric field existing between the tip (1) and the aperture (2) will cause a stream of electrons to be emitted from the tip (1), pass the aperture (2) and to continue as a beam (4) of free electroms beyond said aperture (2). The sheet (3) carrying the aperture (2) may, for example, be a carbon foil or a metallic foil, including gold. The distance of the tip (1) from the aperture (2) is in the submicron range, and so is the diameter of said aperture (2). The distance is being held essentially constant by means of a feedback loop system. The divergence of the beam (4) is

    6.
    发明专利
    未知

    公开(公告)号:DE68917310D1

    公开(公告)日:1994-09-08

    申请号:DE68917310

    申请日:1989-12-13

    Applicant: IBM

    Abstract: The Delta-Phi microlens consists of a first foil (3) of a metal or alloy from the group of transition metals and a second foil (4) of a metal or alloy from the group comprising the elements of IA or IIA groups of the periodic system of elements, the second foil (4) being coated onto one surface of said first foil (3). A hole (2) extends through both foils (3, 4) in precise alignment with the axis (6) of a sharply pointed tip (1) made of conductive material and placed at a distance of the order of 1 mu m from that surface of said first foil (3) opposite said second foil (4). With the first foil (3) connected to ground and a potential on the order of -30 V applied at said tip (1), at ultra-high vacuum conditions, a beam of low-energy electrons will have trajectories (5) deviated towards a focal point (7). With a positive potential of more than 30 V applied to said tip (1), and in a noble gas atmosphere, a beam of ions passing through the microlens of the invention will have trajectories (5) deflected towards said focal point (7).

    7.
    发明专利
    未知

    公开(公告)号:DE3887891D1

    公开(公告)日:1994-03-24

    申请号:DE3887891

    申请日:1988-11-01

    Applicant: IBM

    Abstract: This source for charged particles comprises a sharply pointed tip (1) and an aperture (2) in a thin sheet of material. If the point of the tip (1) is made sharp enough, i.e., if it ends in a single atom or a trimer of atoms, the electric field existing between the tip (1) and the aperture (2) will cause a stream of electrons to be emitted from the tip (1), pass the aperture (2) and to continue as a beam (4) of free electroms beyond said aperture (2). The sheet (3) carrying the aperture (2) may, for example, be a carbon foil or a metallic foil, including gold. The distance of the tip (1) from the aperture (2) is in the submicron range, and so is the diameter of said aperture (2). The distance is being held essentially constant by means of a feedback loop system. The divergence of the beam (4) is

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