Experimental investigation of laser ablation of stone polycrystalline targets

We report the results of an experimental investigation of ablation of stone polycrystalline targets of complex multicomponent composition, which imitate the substance of asteroids. The targets were irradiated by nanosecond pulses of a neodymium laser at an energy density ΦL of up to 5 × 104 J cm−2....

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Veröffentlicht in:Quantum electronics (Woodbury, N.Y.) N.Y.), 2020-08, Vol.50 (8), p.763-769
Hauptverfasser: Burdonskii, I.N., Leonov, A.G., Makarov, K.N., Yufa, V.N.
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creator Burdonskii, I.N.
Leonov, A.G.
Makarov, K.N.
Yufa, V.N.
description We report the results of an experimental investigation of ablation of stone polycrystalline targets of complex multicomponent composition, which imitate the substance of asteroids. The targets were irradiated by nanosecond pulses of a neodymium laser at an energy density ΦL of up to 5 × 104 J cm−2. The experiments demonstrated the existence of two ablation regimes, with the boundary between them lying at ΦL ≈ 4000 J cm−2. The regime change is characterised by a change in the form of the dependence of the surface mass density of removed target material on the laser energy density and by the appearance of a minimum in the dependence of specific energy of destruction on ΦL. This is supposedly related to the passage from a one-dimensional plasma plume expansion to the three-dimensional one and the corresponding decrease in the efficiency of energy transfer from the laser beam to the target due to a lowering of laser-produced plasma density. Our experiments also showed the existence of a maximum in impulse coupling coefficient Cm as a function of laser energy density (Cm ≈ 6.3 × 10−5 N W−1 for ΦL = Φopt ≈ 25 J cm−2). Maxima were also recorded in the dependences of the ablation efficiency and average ablation flow velocity on ΦL. For ΦL > Φopt, the decrease in the function Cm(ΦL) turns out to be much steeper than for metals and polymer materials. The difference is supposedly due to the lower strength and lower plasticity of the polycrystalline stone targets.
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The targets were irradiated by nanosecond pulses of a neodymium laser at an energy density ΦL of up to 5 × 104 J cm−2. The experiments demonstrated the existence of two ablation regimes, with the boundary between them lying at ΦL ≈ 4000 J cm−2. The regime change is characterised by a change in the form of the dependence of the surface mass density of removed target material on the laser energy density and by the appearance of a minimum in the dependence of specific energy of destruction on ΦL. This is supposedly related to the passage from a one-dimensional plasma plume expansion to the three-dimensional one and the corresponding decrease in the efficiency of energy transfer from the laser beam to the target due to a lowering of laser-produced plasma density. Our experiments also showed the existence of a maximum in impulse coupling coefficient Cm as a function of laser energy density (Cm ≈ 6.3 × 10−5 N W−1 for ΦL = Φopt ≈ 25 J cm−2). Maxima were also recorded in the dependences of the ablation efficiency and average ablation flow velocity on ΦL. For ΦL &gt; Φopt, the decrease in the function Cm(ΦL) turns out to be much steeper than for metals and polymer materials. 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The targets were irradiated by nanosecond pulses of a neodymium laser at an energy density ΦL of up to 5 × 104 J cm−2. The experiments demonstrated the existence of two ablation regimes, with the boundary between them lying at ΦL ≈ 4000 J cm−2. The regime change is characterised by a change in the form of the dependence of the surface mass density of removed target material on the laser energy density and by the appearance of a minimum in the dependence of specific energy of destruction on ΦL. This is supposedly related to the passage from a one-dimensional plasma plume expansion to the three-dimensional one and the corresponding decrease in the efficiency of energy transfer from the laser beam to the target due to a lowering of laser-produced plasma density. Our experiments also showed the existence of a maximum in impulse coupling coefficient Cm as a function of laser energy density (Cm ≈ 6.3 × 10−5 N W−1 for ΦL = Φopt ≈ 25 J cm−2). Maxima were also recorded in the dependences of the ablation efficiency and average ablation flow velocity on ΦL. For ΦL &gt; Φopt, the decrease in the function Cm(ΦL) turns out to be much steeper than for metals and polymer materials. The difference is supposedly due to the lower strength and lower plasticity of the polycrystalline stone targets.</description><subject>ABLATION</subject><subject>asteroid deflection</subject><subject>ATOMIC AND MOLECULAR PHYSICS</subject><subject>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS</subject><subject>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</subject><subject>COUPLING</subject><subject>Coupling coefficients</subject><subject>DENSITY</subject><subject>Dependence</subject><subject>EFFICIENCY</subject><subject>ENERGY DENSITY</subject><subject>ENERGY TRANSFER</subject><subject>Flow velocity</subject><subject>Flux density</subject><subject>FUNCTIONS</subject><subject>impulse coupling coefficient</subject><subject>IRRADIATION</subject><subject>Laser ablation</subject><subject>Laser beams</subject><subject>LASER-PRODUCED PLASMA</subject><subject>Lasers</subject><subject>Maxima</subject><subject>Nanosecond pulses</subject><subject>NEODYMIUM LASERS</subject><subject>PLASMA DENSITY</subject><subject>plasma plume</subject><subject>PLASTICITY</subject><subject>POLYCRYSTALS</subject><subject>PULSES</subject><subject>Stone</subject><subject>stone targets</subject><subject>THREE-DIMENSIONAL LATTICES</subject><issn>1063-7818</issn><issn>1468-4799</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNqFkEtLAzEUhYMoWLTgTxjQhZvRJJPnUkp9QEWE7sMkvVNHxsk0ScX-e1OqdiHi6j747uHcg9AZwVcES3z9PJ0RSSU_QCPChCqZ1Pow91hUpVREHaNxjK3FnDHMlVAj9Dj9GCC0b9Cnuiva_h1iapd1an1f-Kbo6gihqG33s4nJ91AMvtu4sIn5qGvznOqwhBRP0VFTdxHGX_UEzW-n88l9OXu6e5jczEpXCZ1Kq4WESjnNFTCtrbScgrUUNw0VjdWMLKTDVgNgImtBlFScyAUBTK1WrjpB5ztZn82a6NoE7sX5vgeXDK0II1rJPTUEv1rnv8yrX4c--zKUZR-Y6Yr9Q1GeoxJb6nJHueBjDNCYIYdWh40h2GyjN9_RZ_Rih7Z-2GutoDMcG2WkqMywaP7Afql9AufqjMo</recordid><startdate>20200801</startdate><enddate>20200801</enddate><creator>Burdonskii, I.N.</creator><creator>Leonov, A.G.</creator><creator>Makarov, K.N.</creator><creator>Yufa, V.N.</creator><general>Kvantovaya Elektronika, Turpion Ltd and IOP Publishing</general><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20200801</creationdate><title>Experimental investigation of laser ablation of stone polycrystalline targets</title><author>Burdonskii, I.N. ; 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Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>Quantum electronics (Woodbury, N.Y.)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Burdonskii, I.N.</au><au>Leonov, A.G.</au><au>Makarov, K.N.</au><au>Yufa, V.N.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Experimental investigation of laser ablation of stone polycrystalline targets</atitle><jtitle>Quantum electronics (Woodbury, N.Y.)</jtitle><addtitle>Quantum Electron</addtitle><date>2020-08-01</date><risdate>2020</risdate><volume>50</volume><issue>8</issue><spage>763</spage><epage>769</epage><pages>763-769</pages><issn>1063-7818</issn><eissn>1468-4799</eissn><abstract>We report the results of an experimental investigation of ablation of stone polycrystalline targets of complex multicomponent composition, which imitate the substance of asteroids. The targets were irradiated by nanosecond pulses of a neodymium laser at an energy density ΦL of up to 5 × 104 J cm−2. The experiments demonstrated the existence of two ablation regimes, with the boundary between them lying at ΦL ≈ 4000 J cm−2. The regime change is characterised by a change in the form of the dependence of the surface mass density of removed target material on the laser energy density and by the appearance of a minimum in the dependence of specific energy of destruction on ΦL. This is supposedly related to the passage from a one-dimensional plasma plume expansion to the three-dimensional one and the corresponding decrease in the efficiency of energy transfer from the laser beam to the target due to a lowering of laser-produced plasma density. Our experiments also showed the existence of a maximum in impulse coupling coefficient Cm as a function of laser energy density (Cm ≈ 6.3 × 10−5 N W−1 for ΦL = Φopt ≈ 25 J cm−2). Maxima were also recorded in the dependences of the ablation efficiency and average ablation flow velocity on ΦL. For ΦL &gt; Φopt, the decrease in the function Cm(ΦL) turns out to be much steeper than for metals and polymer materials. The difference is supposedly due to the lower strength and lower plasticity of the polycrystalline stone targets.</abstract><cop>Bristol</cop><pub>Kvantovaya Elektronika, Turpion Ltd and IOP Publishing</pub><doi>10.1070/QEL17275</doi><tpages>7</tpages></addata></record>
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subjects ABLATION
asteroid deflection
ATOMIC AND MOLECULAR PHYSICS
CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS
CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY
COUPLING
Coupling coefficients
DENSITY
Dependence
EFFICIENCY
ENERGY DENSITY
ENERGY TRANSFER
Flow velocity
Flux density
FUNCTIONS
impulse coupling coefficient
IRRADIATION
Laser ablation
Laser beams
LASER-PRODUCED PLASMA
Lasers
Maxima
Nanosecond pulses
NEODYMIUM LASERS
PLASMA DENSITY
plasma plume
PLASTICITY
POLYCRYSTALS
PULSES
Stone
stone targets
THREE-DIMENSIONAL LATTICES
title Experimental investigation of laser ablation of stone polycrystalline targets
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