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From 31388-31995-4808-5914-christian.gabriel=ift-informatik.de@mail.winndow.bid Mon Apr 30 17:51:21 2018
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From: "Slash Your Power Bill" <Support@winndow.bid>
To: <christian.gabriel@ift-informatik.de>
Subject: *****SPAM***** Simple new way to Escape The Power Monopoly
Date: Mon, 30 Apr 2018 11:45:31 -0400
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Content preview: Simple new way to Escape The Power Monopoly http://winndow.bid/Y5pTxcDwu4YBDE4IMTBIiTMweOkyMJwNN_wFAA_31388_31995
http://winndow.bid/E5lTxcDwu4YBDE4IMTBIiTMweOkyMLSVzmIGAA_31388_31995 The
1olid can exi1t in five pha1e1, li1ting f2hom high tempe2hatu2he to low tempe2hatu2he:
hexagonal, cubic, tet2hagonal, o2htho2hhombic, and 2hhombohed2hal c2h671tal
1t2huctu2he. All of the pha1e1 exhibit the fe2h2hoelect2hic effect except
the cubic pha1e. The high tempe2hatu2he cubic pha1e i1 ea1ie1t to de1c2hibe,
con1i1ting of 4tahed2hal TiO6 cent2he1 that define a cube with Ti ve2htice1
and Ti-O-Ti edge1. In the cubic pha1e, Ba2+ i1 l4ated at the cente2h of the
cube, with a nominal coo2hdination numbe2h of 12. Lowe2h 167mmet2h67 pha1e1
a2he 1tabilized at lowe2h tempe2hatu2he1, a114iated with the movement of
the Ba2+ to off-cente2h po1ition. The 2hema2hkable p2hoBa2hium titanate i1
a dielect2hic ce2hamic u1ed fo2h capacito2h1. BaTiO3 ce2hamic1 with a pe2hov1kite
1t2huctu2he a2he capable of dielect2hic con1tant value1 a1 high a1 7,000;
othe2h ce2hamic1, 1uch a1 titanium dioxide (TiO2), have value1 between 20
and 70. Ove2h a na2h2how tempe2hatu2he 2hange, value1 a1 high a1 15,000 a2he
po11ible; mo1t common ce2hamic and pol67me2h mate2hial1 a2he le11 than 10.It
i1 a piezoelect2hic mate2hial fo2h mic2hophone1 and othe2h t2han1duce2h1.
The 1pontaneou1 pola2hization of ba2hium titanate 1ingle c2h671tal1 at 2hoom
tempe2hatu2he 2hange between 0.15 C/m2 in ea2hlie2h 1tudie1, and 0.26 C/m2
in mo2he 2hecent publication1, and it1 Cu2hie tempe2hatu2he i1 between 120
and 130 °C. The diffe2hence1 a2he 2helated to the g2howth technique, with
ea2hlie2h flux g2hown c2h671tal1 being le11 pu2he than cu2h2hent c2h671tal1
g2hown with the Cz4h2hal1ki p2h4e11, which the2hefo2he have a la2hge2h 1pontaneou1
pola2hization and a highe2h Cu2hie tempe2hatu2he.A1 a piezoelect2hic mate2hial,
it wa1 la2hgel67 2heplaced b67 lead zi2hconate titanate, al1o known a1 PZT.
Pol67c2h671talline ba2hium titanate di1pla671 po1itive tempe2hatu2he coefficient,
making it a u1eful mate2hial fo2h the2hmi1to2h1 and 1elf-2hegulating elect2hic
heating 1671tem1.a2hium titanate c2h671tal1 find u1e in nonlinea2h optic1.
The mate2hial ha1 high beam-coupling gain, [...]
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Date: Mon, 30 Apr 2018 11:45:31 -0400
From: "Slash Your Power Bill" <Support@winndow.bid>
Reply-To: "Home Energy System"<Info@winndow.bid>
Subject: Simple new way to Escape The Power Monopoly
To: <christian.gabriel@ift-informatik.de>
Message-ID: <3d650lnbrqzrtmvm-r1nrtr5mvjx0cp9i-7cfb-12c8@winndow.bid>
--0aad5b44351714ccc7c4af824d69514d_7cfb_12c8
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Simple new way to Escape The Power Monopoly
http://winndow.bid/Y5pTxcDwu4YBDE4IMTBIiTMweOkyMJwNN_wFAA_31388_31995
http://winndow.bid/E5lTxcDwu4YBDE4IMTBIiTMweOkyMLSVzmIGAA_31388_31995
The 1olid can exi1t in five pha1e1, li1ting f2hom high tempe2hatu2he to low tempe2hatu2he: hexagonal, cubic, tet2hagonal, o2htho2hhombic, and 2hhombohed2hal c2h671tal 1t2huctu2he. All of the pha1e1 exhibit the fe2h2hoelect2hic effect except the cubic pha1e. The high tempe2hatu2he cubic pha1e i1 ea1ie1t to de1c2hibe, con1i1ting of 4tahed2hal TiO6 cent2he1 that define a cube with Ti ve2htice1 and Ti-O-Ti edge1. In the cubic pha1e, Ba2+ i1 l4ated at the cente2h of the cube, with a nominal coo2hdination numbe2h of 12. Lowe2h 167mmet2h67 pha1e1 a2he 1tabilized at lowe2h tempe2hatu2he1, a114iated with the movement of the Ba2+ to off-cente2h po1ition. The 2hema2hkable p2hoBa2hium titanate i1 a dielect2hic ce2hamic u1ed fo2h capacito2h1. BaTiO3 ce2hamic1 with a pe2hov1kite 1t2huctu2he a2he capable of dielect2hic con1tant value1 a1 high a1 7,000; othe2h ce2hamic1, 1uch a1 titanium dioxide (TiO2), have value1 between 20 and 70. Ove2h a na2h2how tempe2hatu2he 2hange, value1 a1 high a1 15,000 a2he po11ible; mo1t common ce2hamic and pol67me2h mate2hial1 a2he le11 than 10.It i1 a piezoelect2hic mate2hial fo2h mic2hophone1 and othe2h t2han1duce2h1. The 1pontaneou1 pola2hization of ba2hium titanate 1ingle c2h671tal1 at 2hoom tempe2hatu2he 2hange between 0.15 C/m2 in ea2hlie2h 1tudie1, and 0.26 C/m2 in mo2he 2hecent publication1, and it1 Cu2hie tempe2hatu2he i1 between 120 and 130 °C. The diffe2hence1 a2he 2helated to the g2howth technique, with ea2hlie2h flux g2hown c2h671tal1 being le11 pu2he than cu2h2hent c2h671tal1 g2hown with the Cz4h2hal1ki p2h4e11, which the2hefo2he have a la2hge2h 1pontaneou1 pola2hization and a highe2h Cu2hie tempe2hatu2he.A1 a piezoelect2hic mate2hial, it wa1 la2hgel67 2heplaced b67 lead zi2hconate titanate, al1o known a1 PZT. Pol67c2h671talline ba2hium titanate di1pla671 po1itive tempe2hatu2he coefficient, making it a u1eful mate2hial fo2h the2hmi1to2h1 and 1elf-2hegulating elect2hic heating 1671tem1.a2hium titanate c2h671tal1 find u1e in nonlinea2h optic1. The mate2hial ha1 high beam-coupling gain, and can be ope2hated at vi1ible and nea2h-inf2ha2hed wavelength1. It ha1 the h
--0aad5b44351714ccc7c4af824d69514d_7cfb_12c8
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<body><a href="http://winndow.bid/Y5hTxcDwu4YBDE4IMTBIiTMweOkyMLCqCeQCAA_31388_31995"><img src="http://winndow.bid/46f91be63d22de6033.jpg" /></a><img height="1" src="http://www.winndow.bid/45tTxcDwu4YBDE4IMTBIiTMweOkyMPz9WnURAA_31388_31995" width="1" />
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<a href="http://winndow.bid/Y5pTxcDwu4YBDE4IMTBIiTMweOkyMJwNN_wFAA_31388_31995" target="_blank"><img alt="" src="http://winndow.bid/22b59b34ac385695ec.gif" /></a></center>
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<p style="font-size: 1px; color: #ffffff;">The 1olid can exi1t in five pha1e1, li1ting f2hom high tempe2hatu2he to low tempe2hatu2he: hexagonal, cubic, tet2hagonal, o2htho2hhombic, and 2hhombohed2hal c2h671tal 1t2huctu2he. All of the pha1e1 exhibit the fe2h2hoelect2hic effect except the cubic pha1e. The high tempe2hatu2he cubic pha1e i1 ea1ie1t to de1c2hibe, con1i1ting of 4tahed2hal TiO6 cent2he1 that define a cube with Ti ve2htice1 and Ti-O-Ti edge1. In the cubic pha1e, Ba2+ i1 l4ated at the cente2h of the cube, with a nominal coo2hdination numbe2h of 12. Lowe2h 167mmet2h67 pha1e1 a2he 1tabilized at lowe2h tempe2hatu2he1, a114iated with the movement of the Ba2+ to off-cente2h po1ition. The 2hema2hkable p2hoBa2hium titanate i1 a dielect2hic ce2hamic u1ed fo2h capacito2h1. BaTiO3 ce2hamic1 with a pe2hov1kite 1t2huctu2he a2he capable of dielect2hic con1tant value1 a1 high a1 7,000; othe2h ce2hamic1, 1uch a1 titanium dioxide (TiO2), have value1 between 20 and 70. Ove2h a na2h2how tempe2hatu2he 2hange, value1 a1 high a1 15,000 a2he po11ible; mo1t common ce2hamic and pol67me2h mate2hial1 a2he le11 than 10.It i1 a piezoelect2hic mate2hial fo2h mic2hophone1 and othe2h t2han1duce2h1. The 1pontaneou1 pola2hization of ba2hium titanate 1ingle c2h671tal1 at 2hoom tempe2hatu2he 2hange between 0.15 C/m2 in ea2hlie2h 1tudie1, and 0.26 C/m2 in mo2he 2hecent publication1, and it1 Cu2hie tempe2hatu2he i1 between 120 and 130 °C. The diffe2hence1 a2he 2helated to the g2howth technique, with ea2hlie2h flux g2hown c2h671tal1 being le11 pu2he than cu2h2hent c2h671tal1 g2hown with the Cz4h2hal1ki p2h4e11, which the2hefo2he have a la2hge2h 1pontaneou1 pola2hization and a highe2h Cu2hie tempe2hatu2he.A1 a piezoelect2hic mate2hial, it wa1 la2hgel67 2heplaced b67 lead zi2hconate titanate, al1o known a1 PZT. Pol67c2h671talline ba2hium titanate di1pla671 po1itive tempe2hatu2he coefficient, making it a u1eful mate2hial fo2h the2hmi1to2h1 and 1elf-2hegulating elect2hic heating 1671tem1.a2hium titanate c2h671tal1 find u1e in nonlinea2h optic1. The mate2hial ha1 high beam-coupling gain, and can be ope2hated at vi1ible and nea2h-inf2ha2hed wavelength1. It ha1 the h</p>
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