<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2012.38098</article-id><article-id pub-id-type="publisher-id">JMP-21682</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Matter Waves in a Static Gravitational Field
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>eculai</surname><given-names>Agavriloaei</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>ACK srl, Pascani, Romania</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>naga@ack.ro</email></corresp></author-notes><pub-date pub-type="epub"><day>14</day><month>08</month><year>2012</year></pub-date><volume>03</volume><issue>08</issue><fpage>750</fpage><lpage>754</lpage><history><date date-type="received"><day>May</day>	<month>16,</month>	<year>2012</year></date><date date-type="rev-recd"><day>June</day>	<month>9,</month>	<year>2012</year>	</date><date date-type="accepted"><day>June</day>	<month>30,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  A new approach of the matter waves concept initiated by Louis de Broglie leads to a new model – the vacuum matter waves. By using the physics of time dilation, one can calculate a gravitational cutoff frequency, with respect to the spectrum of vacuum fluctuations, which is the upper bound of the frequency range of this new model. We described the properties of these new waves and outlined the connection between them and the dimensions at Planck length level. The calculation of velocity in circular orbits by using this new concept complies with the well-known equation. One of its consequences is that the structure of the physical vacuum is modified on the radial direction with the gravity source, but not modified on its tangential direction. This study places the space-time structure from sub-quantum level into a new light and makes the connection between this level and that of the planetary systems.
 
</p></abstract><kwd-group><kwd>Matter Waves; Quantum Vacuum; De Broglie Waves; Special Relativity Theory; Inertia; Mach’s Principle</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In 1924, Louis de Broglie in his doctoral thesis “On the Theory of Quanta” [<xref ref-type="bibr" rid="scirp.21682-ref1">1</xref>], claimed the existence of matter waves and formulated the equation that carries his name<img src="12-7500750\96601c0b-80b8-407e-91a4-d05ec95016a2.jpg" />. This hypothesis says that particles of matter have wave-like properties. The concept of matter waves was experimentally confirmed for the first time in 1927 at Bell Labs, by Clinton Davisson and Lester Germer, by using electrons [<xref ref-type="bibr" rid="scirp.21682-ref2">2</xref>]. Recent experiments confirmed the de Broglie equation even for large molecules and macromolecules [3,4].</p><p>On the other hand, the tendency in modern physics, in an effort to unify the fundamental theories, is to find a connection between them and the quantum vacuum. This is the aim of this paper, namely to find out how this vacuum and the concept of matter waves are related.</p><p>The current study is grounded in the basic ideas of de Broglie, but using a new approach. Thus we are led to a new concept—vacuum matter waves—having a deterministic role in the genesis and motion of matter.</p></sec><sec id="s2"><title>2. Vacuum Matter Waves</title><p>In modern physics, the concept of time dilation is a welldocumented physical phenomenon in both theory and experiments. This concept originates in the experiments for ether detection (luminiferous ether), which were initiated in 1887 by Albert Michelson and Edward Morley [<xref ref-type="bibr" rid="scirp.21682-ref5">5</xref>] and continued until recently with the use of lasers and high accuracy devices [<xref ref-type="bibr" rid="scirp.21682-ref6">6</xref>]. The Principle of Invariant Light Speed used by Einstein in his Special Relativity (SR), motivated by Maxwell’s theory of electromagnetism and the lack of evidence for luminiferous ether has as consequences time dilation and length contraction. Velocity and gravitational time dilation have been experimentally confirmed a number of times [7-12].</p><p>As is well known in SR, if the clock has a frequency <img src="12-7500750\ae4fe633-8d3c-47aa-b035-706de69fc02b.jpg" /> (angular frequency) in the rest frame of the particle, its frequency, according to the so-called time dilation, when it is moving with velocity <img src="12-7500750\6c36c87e-b427-4e4f-a41c-cc337ac8cfa8.jpg" /> is:</p><disp-formula id="scirp.21682-formula29547"><label>(1)</label><graphic position="anchor" xlink:href="12-7500750\3cad7806-5fa2-42c3-997e-261be8fa6650.jpg"  xlink:type="simple"/></disp-formula><p>where c<sub>0</sub> denotes the speed of light in a vacuum in the absence of a gravitational field. De Broglie assumed that <img src="12-7500750\2416f2b9-7b20-4df8-b8a1-ad59e7b822dd.jpg" /> is not the frequency of a clock moving with the particle, but the frequency of a wave accompanying the particle, propagating with velocity <img src="12-7500750\e1ff1923-021a-45ba-9a8a-8b5e195a1586.jpg" /> (phase velocity) in the direction of motion (suppose we simplify our 3-dimensional universe to a 1-dimensional universe where we also put in an x-axis). Moreover, in this study we will consider <img src="12-7500750\dc07e61f-8573-47f2-a185-d7619a167c80.jpg" /> as a frequency from the spectrum of vacuum fluctuations. Equation (1) can be rewritten as follows:</p><disp-formula id="scirp.21682-formula29548"><label>(2)</label><graphic position="anchor" xlink:href="12-7500750\15d0450e-0354-46d4-b9c7-a57f94c7d0c7.jpg"  xlink:type="simple"/></disp-formula><p>Also according to de Broglie’s theory, velocity <img src="12-7500750\bc4ae265-113d-454b-890d-8377b2cd2f47.jpg" /> is the group velocity of a wave packet composed of plane waves of a narrow bandwidth. The relation between phase velocity <img src="12-7500750\67f87026-7cae-4773-baeb-a4718c64497a.jpg" /> and group velocity <img src="12-7500750\5cf4407a-6996-4a34-82b5-7b5601352ecb.jpg" /> is given in the Rayleigh equation:</p><disp-formula id="scirp.21682-formula29549"><label>(3)</label><graphic position="anchor" xlink:href="12-7500750\b31cbe5c-5dab-4e9b-a81a-4b689fb7fd27.jpg"  xlink:type="simple"/></disp-formula><p>From Equations (2) and (3) results the following differential equation:</p><disp-formula id="scirp.21682-formula29550"><label>(4)</label><graphic position="anchor" xlink:href="12-7500750\b4ba8361-71be-41c1-afd4-5328cc8dc932.jpg"  xlink:type="simple"/></disp-formula><p>The solution of this equation is:</p><disp-formula id="scirp.21682-formula29551"><label>(5)</label><graphic position="anchor" xlink:href="12-7500750\7999d84b-aaba-4ade-8777-d551ba062077.jpg"  xlink:type="simple"/></disp-formula><p>For avoiding an infinite value, but also for satisfying equation<img src="12-7500750\b2fa9d51-24f7-47ab-a00b-332abaf182d9.jpg" />, we shall consider the solution for which<img src="12-7500750\e4509e4d-5482-461d-af25-4fb79a2301c1.jpg" />. For inserting the influence of the gravitational field in the Equation (5), we shall analyze the relativistic fall (<xref ref-type="fig" rid="fig1">Figure 1</xref>) of a massive particle with mass m in a static gravitational potential <img src="12-7500750\d061d599-492f-4a53-935e-ca6b29e43170.jpg" /> generated by mass<img src="12-7500750\ef92e279-5d2c-404d-9b2c-702f70e6cb50.jpg" />.</p><p>This particle comes from an infinite distance (<img src="12-7500750\fbca6cc2-50af-4610-9e6d-a76d661f7ceb.jpg" />) with initial velocity<img src="12-7500750\74144498-d05d-430a-8c8d-a465f63918ed.jpg" />. Taking into account the gravitational potential<img src="12-7500750\7f442792-6b84-4232-a4e6-60e0f0d477ac.jpg" />, the relativistic velocity satisfies the following equation:</p><disp-formula id="scirp.21682-formula29552"><label>(6)</label><graphic position="anchor" xlink:href="12-7500750\ac3766ee-a3b5-42bc-9255-02eb3526d032.jpg"  xlink:type="simple"/></disp-formula><p>For the multibody potential, <img src="12-7500750\8bc313fa-23a2-4491-864a-b1710ad1f914.jpg" />represents the sum of the Newtonian gravitational potentials due to the masses in the neighborhood.</p><disp-formula id="scirp.21682-formula29553"><label>(7)</label><graphic position="anchor" xlink:href="12-7500750\f9e3fe13-40dc-4857-a85d-9794679bf3e6.jpg"  xlink:type="simple"/></disp-formula><p>If considering Equation (1), Equation (6) is written as follows:</p><disp-formula id="scirp.21682-formula29554"><label>(8)</label><graphic position="anchor" xlink:href="12-7500750\3e5efebc-0a18-46dc-89f6-f01305268c51.jpg"  xlink:type="simple"/></disp-formula><p>This equation can be rewritten in a simplified form as follows:</p><disp-formula id="scirp.21682-formula29555"><label>(9)</label><graphic position="anchor" xlink:href="12-7500750\8c8816c6-283f-4c0e-b63e-918ecc6b7f26.jpg"  xlink:type="simple"/></disp-formula><p>in which we made the following denotation:</p><disp-formula id="scirp.21682-formula29556"><label>(10)</label><graphic position="anchor" xlink:href="12-7500750\b7db24e8-2571-4cd9-a705-335840a0d406.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="12-7500750\a36fe32b-3e31-43f6-8dd8-7f6a573f3343.jpg" /> is the frequency from the spectrum of vacuum fluctuations, in which the group velocity is null.</p><p>The phase velocity can likewise be computed in the way we obtained Equation (5):</p><disp-formula id="scirp.21682-formula29557"><label>(11)</label><graphic position="anchor" xlink:href="12-7500750\a4213196-5665-49ed-beac-222057b605bd.jpg"  xlink:type="simple"/></disp-formula><p>As can be seen in <xref ref-type="fig" rid="fig2">Figure 2</xref>, the range of frequencies <img src="12-7500750\f2395874-ccaf-460e-ac19-5481819cbbd0.jpg" /> does cover the entire range that is necessary for generating the group velocities<img src="12-7500750\665747b8-f496-4486-86b0-db759ff8a230.jpg" />.</p><p>The value <img src="12-7500750\a6c49c5c-101d-411e-ae5a-b70600026438.jpg" /> can be interpreted as a gravitational cutoff frequency, so that frequencies spectrum of vacuum fluctuations that may participate in the formation of the massive particles are in the range<img src="12-7500750\ab297685-9439-4d41-bfc7-4c771638462a.jpg" />. Observe that as gravitational field strength is higher so the cutoff frequency is higher. We can interpret this fact as under the influence of gravity, a part of the frequency spectrum that is present in vacuum fluctuations is extracted and used in the genesis and motion of the matter. In the absence of gravity, the cutoff frequency has an initial value<img src="12-7500750\eaaf6d49-74e1-4dae-9d41-a9006055deee.jpg" />. Further, we call these waves having the phase velocity <img src="12-7500750\0315e508-4317-42fc-b3fa-60f600f52599.jpg" /> and frequencies in the range of <img src="12-7500750\0c685912-3829-4f89-a926-6457083ef2b6.jpg" /> as vacuum matter waves.</p></sec><sec id="s3"><title>3. Properties of Vacuum Matter Waves</title><p>We can split the range of frequencies <img src="12-7500750\aae3f203-d8eb-4887-ae86-f946d92b4867.jpg" /> by the value of the group velocity V relative to the escape velocity<img src="12-7500750\c88b6885-ad31-490d-b9a1-8cdb091da58b.jpg" />. Thus, for a frequency<img src="12-7500750\27b0fb72-e2d4-4c0f-8ce6-410678addc33.jpg" />, the group velocity is equal to the escape velocity. For the range of frequencies lower than<img src="12-7500750\807755fd-e3f0-4ce3-bbb6-5e8be5256e68.jpg" />, the group velocity is higher than the escape velocity, while for the range of <img src="12-7500750\6a0b14c9-3a6a-4c8f-9e14-880959828504.jpg" /> the group velocity is lower than the escape velocity.</p><disp-formula id="scirp.21682-formula29558"><label>(12)</label><graphic position="anchor" xlink:href="12-7500750\566ee494-f180-4a19-b397-59249d5e9f87.jpg"  xlink:type="simple"/></disp-formula><p>For vacuum matter waves, the upper limit of the phase velocity is<img src="12-7500750\3c3bc695-f003-4070-a010-e34d7a101aad.jpg" />, and this holds for relatively low frequencies:</p><disp-formula id="scirp.21682-formula29559"><label>(13)</label><graphic position="anchor" xlink:href="12-7500750\9828cccc-ef9a-48e8-a1e8-673674e55475.jpg"  xlink:type="simple"/></disp-formula><p>We can also observe that for a null group velocity, the phase velocity has a fixed value regardless of the of the gravitational field strength:</p><disp-formula id="scirp.21682-formula29560"><label>(14)</label><graphic position="anchor" xlink:href="12-7500750\adc3206d-cdc3-48e5-b10d-f26bde60a6b9.jpg"  xlink:type="simple"/></disp-formula><p>De Broglie-Einstein velocity equation (an equivalent equation) is:</p><disp-formula id="scirp.21682-formula29561"><label>(15)</label><graphic position="anchor" xlink:href="12-7500750\e6c6c8d2-5df0-4037-8453-3759e17f10c8.jpg"  xlink:type="simple"/></disp-formula><p>and has the following property:</p><disp-formula id="scirp.21682-formula29562"><label>(16)</label><graphic position="anchor" xlink:href="12-7500750\41d69e22-dc13-4864-858d-3c9a0564b454.jpg"  xlink:type="simple"/></disp-formula><p>In a static gravitational field the refractive index <img src="12-7500750\e892885f-d303-4b5a-8584-42f022296ced.jpg" /> for vacuum matter waves is:</p><disp-formula id="scirp.21682-formula29563"><label>(17)</label><graphic position="anchor" xlink:href="12-7500750\dc3026a4-8cde-4403-be3c-a9c6409a9e04.jpg"  xlink:type="simple"/></disp-formula><p>The graphical form (<xref ref-type="fig" rid="fig2">Figure 2</xref>) of the phase velocity <img src="12-7500750\b424ff75-5dfa-492b-896c-419396a07e43.jpg" /> around the gravitational cutoff frequency <img src="12-7500750\527c89c7-9a4e-4678-a317-1a048d93d3ab.jpg" /> suggests that there exists a minimal value of the wavelength <img src="12-7500750\25b6c321-8ad4-41c6-ad39-8b4f3dc5feae.jpg" /> for which vacuum matter waves do exist. Thus, we can deduce a value for <img src="12-7500750\63481e3a-caea-4a0d-a1dc-95163230f9fb.jpg" /> from the following equation:</p><disp-formula id="scirp.21682-formula29564"><label>(18)</label><graphic position="anchor" xlink:href="12-7500750\318e0bf2-70eb-4d86-9c3b-65a82ce4d73f.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.21682-formula29565"><label>(19)</label><graphic position="anchor" xlink:href="12-7500750\2cefc1cb-e8de-45d3-9cc4-6ccc6575e637.jpg"  xlink:type="simple"/></disp-formula><p>Equations (10) and (14) yield the minimal value of the wavelength <img src="12-7500750\c67c9280-0262-4890-99ba-cd30c42a212b.jpg" /> as a function of the gravitational potential:</p><disp-formula id="scirp.21682-formula29566"><label>(20)</label><graphic position="anchor" xlink:href="12-7500750\e110ee81-91be-4513-84ef-8c1db3d41ec7.jpg"  xlink:type="simple"/></disp-formula><p>From this equation, it follows that the gravitational potential “deforms” the structure of the physical vacuum, leading to a minimal wavelength<img src="12-7500750\e18f2298-a63e-474e-8f33-44516b1ff647.jpg" />. The vacuum matter waves do not exist below this value.</p><p>We could speculate that <img src="12-7500750\54f67a3b-5e17-4771-9a54-67cf0b594446.jpg" /> has the Planck length, defined as:</p><disp-formula id="scirp.21682-formula29567"><label>(21)</label><graphic position="anchor" xlink:href="12-7500750\72fe02e7-a9b5-46b2-a97c-88e4bf8044c7.jpg"  xlink:type="simple"/></disp-formula><p>In this case, we can compute the initial value of the cutoff frequency by using Equation (19):</p><disp-formula id="scirp.21682-formula29568"><label>(22)</label><graphic position="anchor" xlink:href="12-7500750\2738b352-11f1-46bd-a7a6-199e67ac784d.jpg"  xlink:type="simple"/></disp-formula><p>A brief characterization of the vacuum matter waves in a 1-dimensional universe can be done through the following equations (see <xref ref-type="table" rid="table1">Table 1</xref>).</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Vacuum matter waves properties</title></caption></table-wrap-group></sec><sec id="s4"><title>4. Escape Velocity</title><p>For the escape velocity<img src="12-7500750\387cce52-922b-43b4-8aaa-26626703b463.jpg" />, the wave packet is centered on frequency<img src="12-7500750\9fba4bca-7f0d-4062-a368-c704c3630d2e.jpg" />. The value of this velocity can be computed through Equation (8) as follows:</p><disp-formula id="scirp.21682-formula29569"><label>(23)</label><graphic position="anchor" xlink:href="12-7500750\71e047cf-74df-49fa-8c44-88c3407e040a.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Circular Orbit Velocity</title><p>Denote by <img src="12-7500750\7a1e034a-a42b-4c4d-86f9-5c7b4562ff86.jpg" /> the central frequency of a wave packet moving on a circular orbit with velocity</p><p><img src="12-7500750\76f71aa4-0f10-41fd-b10e-e5382ac5ad9e.jpg" />.</p><p>The wavelength of vacuum matter waves corresponding to this frequency is:</p><disp-formula id="scirp.21682-formula29570"><label>(24)</label><graphic position="anchor" xlink:href="12-7500750\6027510b-6a8b-4e46-a0cf-2a74e299c9ab.jpg"  xlink:type="simple"/></disp-formula><p>We impose the condition of stability of the circular orbit,</p><disp-formula id="scirp.21682-formula29571"><label>(25)</label><graphic position="anchor" xlink:href="12-7500750\8af64448-7f1a-4f24-b4c5-bbea7ba8bd4a.jpg"  xlink:type="simple"/></disp-formula><p>which leads us to the following equation:</p><disp-formula id="scirp.21682-formula29572"><label>(26)</label><graphic position="anchor" xlink:href="12-7500750\f04e711d-2cd5-4b37-967c-ccda2de0022f.jpg"  xlink:type="simple"/></disp-formula><p>This equation can be solved by means of approximate methods using mathematical software. For <img src="12-7500750\33ace36b-2d12-4526-b649-748118536c1b.jpg" /> and<img src="12-7500750\301a3d58-b172-41a9-9f0f-d7fe1967d78d.jpg" />, one of these approximated solutions is:</p><disp-formula id="scirp.21682-formula29573"><label>(27)</label><graphic position="anchor" xlink:href="12-7500750\6a9aed1c-1743-4e89-a047-6b966fd8d5b8.jpg"  xlink:type="simple"/></disp-formula><p>We can compute the circular orbit velocity by using Equation (8):</p><disp-formula id="scirp.21682-formula29574"><label>(28)</label><graphic position="anchor" xlink:href="12-7500750\04d5d2d6-89da-47a3-9870-3281cd325e0f.jpg"  xlink:type="simple"/></disp-formula><p>that is the well-known nonrelativistic value of this velocity. Obtaining the equation of the orbital velocity is of the utmost importance, because it confirms this study.</p><p>The stability condition (25) has been considered as a necessity of a synchronism between the wavelength <img src="12-7500750\87149f51-dc31-4ba8-8e8e-878a7d0505a0.jpg" /> corresponding to the velocity of the motion and the wavelength <img src="12-7500750\e48ead2d-70c6-4b24-8485-63f4e73d983d.jpg" /> characterizing the physical vacuum. A consequence of obeying this condition is the fact that the gravitational potential “deforms” the physical vacuum on the radial direction with the gravity source, but not on its tangential direction.</p></sec><sec id="s6"><title>6. Inertia and Gravity: The Same Phenomenon</title><p>The similarity between (2) and (9) and also between (5) and (11) suggests the fact that as gravitational cutoff frequency <img src="12-7500750\3ae5cf79-7daa-4ea9-bf35-0dd35f759471.jpg" /> is generated by a gravitational potential<img src="12-7500750\55d37ed6-af05-44b7-90ca-6a14ad72f11c.jpg" />, so <img src="12-7500750\23de5c25-475e-43c6-bed8-4a920fabdb03.jpg" /> could be generated by a default gravitational potential<img src="12-7500750\038c7b45-ace8-43f8-abf9-cc8668105598.jpg" />. Thus, the total gravitational potential has the following equation:</p><disp-formula id="scirp.21682-formula29575"><label>(29)</label><graphic position="anchor" xlink:href="12-7500750\4f7a9496-22ef-40f2-9d6a-d54514f204d1.jpg"  xlink:type="simple"/></disp-formula><p>In this case, equation (10) is just an approximation of the cutoff frequency <img src="12-7500750\26329a33-9914-429c-805c-06bd0b2de243.jpg" /> around the value <img src="12-7500750\5c18378d-bee8-49eb-a613-0d7c2cc6b1a0.jpg" /> and we should find a function of the form:</p><disp-formula id="scirp.21682-formula29576"><label>(30)</label><graphic position="anchor" xlink:href="12-7500750\8a0a4071-1bbc-41ff-9608-06fc69ef9789.jpg"  xlink:type="simple"/></disp-formula><p>Gravitational potential <img src="12-7500750\7dab77be-fd7f-4454-afc4-85bcefa36166.jpg" />is generated by all the mass-energy in the entire universe and inertia depends on it [<xref ref-type="bibr" rid="scirp.21682-ref13">13</xref>]. To illustrate the above, in a simplified model, we consider that all mass-energy <img src="12-7500750\77216aab-bda3-4ec8-a10a-bc0f50917c0b.jpg" /> of the universe is distributed uniformly on a thin spherical shell of radius <img src="12-7500750\27d228d6-4ac4-4673-b0f6-9a43fb9447f7.jpg" /> (<xref ref-type="fig" rid="fig3">Figure 3</xref>). Gravitational potential generated by the universe is constantly all the volume.</p><disp-formula id="scirp.21682-formula29577"><label>(31)</label><graphic position="anchor" xlink:href="12-7500750\ea4a2e9c-e001-40e8-bf55-cb4083297794.jpg"  xlink:type="simple"/></disp-formula><p>A mass M located inside the sphere generates a gravitational potential:</p><disp-formula id="scirp.21682-formula29578"><label>(32)</label><graphic position="anchor" xlink:href="12-7500750\d85fdc9b-cbda-4320-9220-47e76bc436b8.jpg"  xlink:type="simple"/></disp-formula><p>Total gravitational potential inside the sphere is:</p><disp-formula id="scirp.21682-formula29579"><label>(33)</label><graphic position="anchor" xlink:href="12-7500750\03a71ce4-1712-4a4e-9e1d-0fbb61066352.jpg"  xlink:type="simple"/></disp-formula><p>If we define the space <img src="12-7500750\f66e72e1-369a-4f52-a5a2-9fb5ad1c0f13.jpg" /> inside the sphere, a test mass m located in a certain place into this space will have a well-defined velocity. In other words, the particle velocity, which is given by the group velocity</p><p><img src="12-7500750\9b72a310-79cb-480a-88be-91203228552a.jpg" />is a property of the space but not the test mass. In this space if<img src="12-7500750\76437b50-65d9-4f11-bacc-74e94c46f30d.jpg" />, the motion of the test mass is inertial<img src="12-7500750\af352d77-d20a-4a11-8b22-552610ceb2a1.jpg" />. If<img src="12-7500750\d8fc80fa-841a-4f04-822b-8140644b0b83.jpg" />, the motion is produced under the influence of an supplementary gravitational potential<img src="12-7500750\3e689cb7-b2c5-4346-8478-a41c5f3a8509.jpg" />. We conclude that in this space, the group velocity <img src="12-7500750\ad19e572-43ed-4268-809b-3907ef350e82.jpg" /> depends on a unique gravitational potential <img src="12-7500750\ad35043d-d6c8-41d8-9ba9-38efed1584b0.jpg" /> does not distinguish between inertial motion and a motion near a mass M.</p><disp-formula id="scirp.21682-formula29580"><label>(34)</label><graphic position="anchor" xlink:href="12-7500750\4b379bc7-92e0-4af4-ac50-1019979db186.jpg"  xlink:type="simple"/></disp-formula><p>From this point of view, inertia and gravitation are the same phenomenon.</p></sec><sec id="s7"><title>7. Compton Frequency and De Broglie Equation</title><p>The nature of the Compton frequency must be the same as the vacuum matter waves. It would be complicated to consider that it would have another origin. One of the possibilities is that Compton frequency <img src="12-7500750\c6047ea6-ed87-4772-a0ab-e8300964ec27.jpg" /> be given by a narrow bandwidth <img src="12-7500750\e46156a4-1fdd-477e-a566-de87424e38eb.jpg" /> of a wave packet, centered on frequency<img src="12-7500750\a42402a2-a99c-4a5e-8155-d143a767c0bc.jpg" />, with the following equation:</p><disp-formula id="scirp.21682-formula29581"><label>(35)</label><graphic position="anchor" xlink:href="12-7500750\e2ede892-8f0e-4885-9226-008687caf501.jpg"  xlink:type="simple"/></disp-formula><p>Of course, <img src="12-7500750\873a94c8-1062-4670-8040-ccfac343c095.jpg" />is the frequency you see in the reference frame of the particle. If the particle moves with velocity<img src="12-7500750\73558a08-771a-4862-90c2-5510f739ad1d.jpg" />, then this frequency changes according to the value:</p><disp-formula id="scirp.21682-formula29582"><label>(36)</label><graphic position="anchor" xlink:href="12-7500750\c7e99530-10ed-4dc0-bd83-7f176f779a8a.jpg"  xlink:type="simple"/></disp-formula><p>The associated wavelength is given by the de Broglie equation <img src="12-7500750\e1b44474-3beb-4653-a897-305d53ed85e9.jpg" /> This way of interpreting the Compton frequency would also justify the equation of energy:</p><disp-formula id="scirp.21682-formula29583"><label>(37)</label><graphic position="anchor" xlink:href="12-7500750\81fd378c-000d-45d7-a287-1240c899158c.jpg"  xlink:type="simple"/></disp-formula><p>given that the energy of a harmonic oscillator is proportional to the square of its frequency.</p></sec><sec id="s8"><title>8. Conclusions</title><p>Using a new approach of the matter waves concept initiated by Louis de Broglie we have build a new model— the vacuum matter waves. For this new model we have calculated the upper limit of the frequency spectrum (gravitational cutoff frequency) as well as some properties. This allows us to get the following conclusions:</p><p>-&#160;&#160;&#160;&#160;&#160;&#160; there is a close deterministic (non probabilistic) relationship between matter, vacuum matter waves and quantum vacuum;</p><p>-&#160;&#160;&#160;&#160;&#160;&#160; there is a gravitational cutoff frequency regarding vacuum fluctuations;</p><p>-&#160;&#160;&#160;&#160;&#160;&#160; this new model makes the connection between Planck level and that of the planetary systems;</p><p>-&#160;&#160;&#160;&#160;&#160;&#160; the space-time is not continuous but discrete;</p><p>-&#160;&#160;&#160;&#160;&#160;&#160; inertia and gravity are the same phenomenon.</p></sec><sec id="s9"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.21682-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">L. De Broglie, “On the Theory of Quanta,” English Trans- lation by A. F. Kracklauer, Annales Fondation Louis de Broglie, 2004.</mixed-citation></ref><ref id="scirp.21682-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">C. Davisson and L. H. Germer, “The Scattering of Elec- trons by a Single Crystal of Nickel,” Nature, Vol. 119, 1927, pp. 558-560. doi:10.1038/119558a0</mixed-citation></ref><ref id="scirp.21682-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">M. Arndt, O. Nairz, J. Voss-Andreae, C. Keller, G. van der Zouw and A. Zeilinger, “Wave-Particle Duality of C60 Molecules,” Nature, Vol. 401, 1999, pp. 680-682. doi:10.1038/44348</mixed-citation></ref><ref id="scirp.21682-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">S. Gerlich, S. Eibenberger, M. Tomandl, S. Nimmrichter, K. Hornberger, P. J. Fagan, J. Tüxen, M. Mayor and M. Arndt, “Quantum Interference of Large Organic Mole- cules,” Nature Communications, Vol. 2, No. 263, 2011, Article ID: 263. doi:10.1038/ncomms1263</mixed-citation></ref><ref id="scirp.21682-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">A. A. Michelson and E. W. Morley, “On the Relative Motion of the Earth and the Luminiferous Ether,” Ameri- can Journal of Science, Vol. 34, No. 203, 1887, pp. 333- 345. </mixed-citation></ref><ref id="scirp.21682-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">H. Muller, et al., “Modern Michelson-Morley Experiment Using Cryogenic Optical Resonators,” 2003.  
http://arxiv.org/abs/physics/0305117</mixed-citation></ref><ref id="scirp.21682-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">H. E. Ives and G. R. Stilwell, “An Experimental Study of the Rate of a Moving Clock,” Journal of the Optical So- ciety of America, Vol. 28, 1938, pp. 215-226. doi:10.1364/JOSA.28.000215</mixed-citation></ref><ref id="scirp.21682-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">H. E. Ives and G. R. Stilwell, “An Experimental Study of the Rate of a Moving Clock,” Journal of the Optical So- ciety of America, Vol. 31, 1941, pp. 369-374. doi:10.1364/JOSA.31.000369</mixed-citation></ref><ref id="scirp.21682-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">B. Rossi and D. B. Hall, “Variation of the Rate of Decay of Mesotrons with Momentum,” Physical Review, Vol. 59, No. 3, 1941, pp. 223-229. doi:10.1103/PhysRev.59.223</mixed-citation></ref><ref id="scirp.21682-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">C. W. Chou, D. B. Hume, T. Rosenband and D. J. Wine- land, “Optical Clocks and Relativity,” Science, Vol. 329 No. 5999, 2010, pp. 1630-1633. doi:10.1126/science.1192720</mixed-citation></ref><ref id="scirp.21682-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">R. V. Pound and G. A. Rebka Jr., “Gravitational Red- Shift in Nuclear Resonance,” Physical Review Letters, Vol. 3 No. 9, 1959, pp. 439-441. doi:10.1103/PhysRevLett.3.439</mixed-citation></ref><ref id="scirp.21682-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">J. Hafele and R. Keating, “Around the World Atomic Clocks: Predicted Relativistic Time Gains,” Science, Vol. 177, No. 4044, 1972, pp. 166-168. doi:10.1126/science.177.4044.166</mixed-citation></ref><ref id="scirp.21682-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">D. W. Sciama, “The Physical Foundations of General Relativity,” Heinemann Educational Books Ltd., London, 1969.</mixed-citation></ref></ref-list></back></article>