It is suggested to teleport particles by creating a cloud of artificial holes around them using the processes of annihilation of pairs particle-antiparticle, decay of true neutral particles and non-elastic scattering. There is probability that the cloud of holes will spontaneously close with instantaneous teleportation of inside particles. In order to prove hole teleportation it is enough to prove the fact of acceleration of particles by holes (levitation).

        For teleportation by hole method it is necessary to send a particle outside of the Universe or to curve space-time in such a way that points of start and finish coincided. It is necessary to create around a particle non-Euclidean geometry, which is named a model of non-Euclidean Universe of Poincare. The simplest method of teleportation not requiring any equipment is natural teleportation. It is necessary to watch a chosen particle. As virtual vacuum holes permanently appear in vacuum, there exist probability that as a result of fluctuations of vacuum there may spontaneously appear a closed hole surface with instantaneous teleportation of inside particles. The smaller are sizes of a body, the higher is probability of teleportation.  For increase of probability of teleportation such places should be found where the number of vacuum holes is higher or to create vacuum holes artificially.
     Nevertheless, expectation time of natural teleportation for macroscopic bodies can exceed the age of the Universe. Therefore it is better to create holes artificially around the target. The more holes are created and the nearer they are placed to some arbitrary closed surface, the higher is probability of teleportation. At creation of closed continuous hole surface around body, the expectation time will be equal to zero.

     Vacuum holes can be created artificially by three methods published in 1994 [1,2,3,4]. These are annihilation of pairs particle-antiparticle, decay of true neutral particles and movement of bodies with acceleration (elastic and inelastic scattering). At inelastic scattering, particles extend vacuum holes creating large holes extended on the line of movement. Thus in the centre of collision of particle beams a cloud of artificial holes is created. There is probability that inside the cloud may appear spontaneously a closed hole surface with instantaneous teleportation of random particles. To increase sizes of vacuum holes, it is better to collide antiparticles, for instance electron-positron beams.
       Since colliders able to create a hole cloud for a long time, it allows us to hope that teleportation of particles will really occur even if a hole cloud is insufficiently dense. In standard collider experiments with inelastic scattering the probability of teleportation is little because the created cloud is non-voluminous. In other words along the trajectory of each of particles is created one, seldom two holes in points of collision.  If we connect by imaginary line all points of collision of particles for one moment of time, then it will be curvilinear flatform surface with very small probability of of closing. The probability of spontaneous closing will be high only in spatially distributed cloud of holes which can be obtained for instance by collision of several particle beams under different angles or by combining various methods of creating of holes. Thus under notion of teleportation of particle in scattering experiments we understand disappearance of one or more colliding particles. We may use all conservation laws for registration of teleportation events. It are energy and charge (electric, baryon, lepton) conservation laws. It is necessary to measure energy or charge of entering (E1) in zone of collisions and outcoming (E2) stream of particles. If E2 will be less than E1 even on value of elementary charge or rest mass of lightest of particles of experiment, then it can mean teleportation only. Disappearance of particles in monitored volume cannot have another explanation but teleportation. The errors like absorption of particles by the chamber or other solid parts of collider must be eliminated or taken into account.

      A teleported particle appears in a random point of the Universe, which is rather beyond the horizon of the visible Universe. The address teleportation is more complicate therefore will be verified latter.
    To check detectors, we may measure E1 and E2 under conditions when teleportation is not possible (When all points of collision lay on a flat surface), therefore E1 must be equal to E2.  To improve the precision of measurement, it is better to chose conditions of experiment with minimal birth of ghost particles like neutrino.
    At inelastic scattering the events of teleportation occurs after long time work of equipment, because it is very rare process.
    Other methods of teleportation may use the decay of true neutral particles or annihilation of pairs particle-antiparticle. For example at irradiation of particle-target with true neutral particles, a cloud of artificial vacuum holes appears around it. There is probability of spontaneous closing of hole cloud with instantaneous teleportation of random particles.
    Example of unconditional teleportation of heavy nuclei.  Here heavy nucleuses are irradiated by a beam of slow antinucleons. The main condition for teleportation is that all nucleons of outer nucleus layer must annihilate simultaneously. Then around nucleus appears a small closed hole surface with instant and unconditional teleportation of rest of nucleus. As things stand would be possible to teleport heavy nuclei consisting of tens or hundreds of nucleons, with expectation time equal to zero. Teleportation event here is absence of a nucleus and simultaneous registration of a number of annihilations equal to the number of nucleons in the outer nucleus layer.
    The most simple way to prove hole teleportation is experimental demonstration of hole levitation.  For it is enough to prove that particles can be accelerated by vacuum holes.
    Teleportation and levitation are connected by strong symmetry - these are superanalogues respectively of uniform rectilinear motion and motion with acceleration which repeats its properties. For example we revealed a massive body capable of moving with acceleration. Does it not mean that this body can also move uniformly-rectilinearly? Symmetrically, experimental demonstration of levitation automatically means that also more complicated hole teleportation is possible. If it is proved existence of superanalogue of motion with acceleration (hole levitation), it automatically means existence of superanalogue of uniform rectilinear motion (hole teleportation).
    For demonstration of hole levitation it is necessary to prove that particles can be accelerated by vacuum holes. It is important to distinguish two cases, when a formed artificial hole "comes in touch" with a particle and when not. At the first case a particle is accelerated by strong interaction, in the second by gravitational. Though both cases are fit for proof, the second case should be considered true levitation. The example of strong levitation is elastic scattering. Particles collide expanding vacuum holes, then they in their turn accelerate them. Respectively at strong levitation particles get bigger impulses, and at gravitational levitation much less.
    For demonstration of gravitational levitation an artificial holes should be created by means of colliding particles, annihilation of pairs or decay of true neutral particles. If particle-detector will move with acceleration by help of vacuum holes, it will be experimental demonstration of hole levitation and hole teleportation. Actually it is verification of hole gravitation. For a short time an artificial gravitational field is created and it is necessary to prove that nearby particle freely fall to the hole. It can be done by irradiating light nucleus, for example deuterium or tritium by slow antineutrons. After annihilation of a neutron from nucleus will appear a vacuum hole which can accelerate the rest of nucleus or can create new particles. It is necessary to measure the impulse of a nucleus after annihilation and to prove that it was accelerated by a hole, but not by other force fields or by collision with other particles. Another similar experiment can be with irradiation of particle-detector by slow true neutral particles, for example by neutral pi mesons. The distance between source and target must satisfy condition that most of particles must decay near target with creation of artificial holes.  It is necessary to prove that particle-target was accelerated by a hole but not by collision or external force fields.
         The levitation will be proved by the following  signs: 1. If particle-detector got an impulse without collision (interaction) with other particles that can be find by analyzing trajectories, energies and impulses of all interacted particles, products of decay, annihilation or non-elastic scattering.  All force fields able to influence motion of particle-detector should be taken into account or must be absent. Such events should be selected where for instance products of decay fly away without interaction with a particle-detector. 2. If the impulse of detector after collision differs from theory. 3. If at detection of particles with high time resolution was found that a particle detector got an impulse before collision, which cannot be explained by action of force fields. 4. At gravitational levitation may be violation of impulse conservation law because the absent impulse was carried out by gravitational waves to surrounding stars and is too small to be detected. We do not know if gravity has classical or quantum properties at this short distances. For example, the following case is possible: the appearance of artificial vacuum hole may cause emission of two holes in opposite directions. If a detector lay on hole trajectory, the hole (or gravitational impulse) will be registered, if particle do not lay on hole trajectory, the gravitational impulse is not registered.
    These experiments can prove hole levitation, teleportation, gravitation and the finite volume of Universe.

 References

1. Leshan C.Z., - The combination of gravitational, strong and weak interaction in hole vacuum and matter, Conference proceedings, ICPS94 S. Petersburg, 1994, 2. Leshan C.Z., The combination of gravitational, strong and weak interaction in hole vacuum and matter, Hole physics, teleportation and levitation. N2, 2002.
3. Leshan C.Z - Combination of gravitational, strong and weak interaction in hole vacuum and matter, str. August 31, 22 Balti, 1994
4. Conference proceedings, ICPS ’ 95, Copenhagen, 1995