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Creep in One Dimension and Phenomenological Theory of Glass Dynamics

Creep in One Dimension and Phenomenological Theory of Glass Dynamics
Creep in One Dimension and Phenomenological Theory of Glass Dynamics

a r X i v :c o n d -m a t

/9

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1131v 2 28 J u l 1995

Creep in One Dimension and Phenomenological Theory of Glass Dynamics

Pierre Le Doussal (1,3,?)and Valerii M.Vinokur (2,3)

(1)

CNRS-Laboratoire de Physique Th′e orique de l’Ecole Normale Sup′e rieure,24rue Lhomond,F-75231Paris

(2)

Materials Science Division,Argonne National Laboratory,Argonne IL 60439

(3)

ITP,University of California,Santa Barbara CA 93106

(February 1,2008)

The dynamics of a glass transition is discussed in terms of the motion of a particle in a one dimensional correlated random potential.An exact calculation of the velocity V under an applied force f demonstrates a variety of dynamic regimes depending on the range of correlations.In a gaussian potential with correlator C (x )=x γ,we ?nd a transition from ohmic behaviour (γ<0)to creep motion V ~exp(?const/f μ)(0<γ<1).This provides a generic picture of the glass transition in systems where long range correlations in the e?ective disorder develop due to elasticity such as elastic manifolds subject to quenched disorder and the vortex glass transition in superconductors.74.60.Ge,05.20.-y

The driven dynamics of physical systems which can be modelled as elastic manifolds in quenched random media has received a lot of attention recently.Prominent exam-ples of such systems are the roughening of domain walls [1],directed polymer growth [2],motion of dislocations in disordered media [3],dynamics of charge density waves [4],and surface growth in a random environment [5].This recent interest was partly motivated by extensive studies of vortex dynamics in high-Tc superconductors.It was shown that this problem is related to the dynamics of an elastic manifold subject to quenched disorder [6–9],

and a signi?cant progress in qualitative understanding was achieved.The motion is viewed as a sequence of thermally activated jumps of the optimal ”cell”of the manifold from one metastable state to the next as fa-vored by the applied force.In most of these systems the activation barriers for such a motion,which we will refer to as creep motion,depends on the applied force f and diverges as f →0,giving rise to a strongly non linear velocity versus applied force dependence.The un-limited growth of the creep barriers is taken now as the characteristic feature and operational de?nition of glassy https://www.doczj.com/doc/ea16557196.html,ually [8]the barriers grow as U B (f )~f ?μleading to a typical velocity vs applied force dependence

(or I-V curve)of the form V =e ?1/(T f μ

)in the creep regime.

While there is now a consistent qualitative picture of the low temperature creep motion [10,6],it is based mostly on scaling arguments and numerical simulations,and a rigorous analysis is still lacking.Although inter-esting new results have been obtained recently for the non-equilibrium dynamics of mean ?eld models of glasses [11]and for particle dynamics in an in?nite-dimensional random potential [12,13],a general analytical derivation in physical models remains an unsolved problem.In the absence of a rigorous analysis of realistic physical

situations one is seeking for models which are simple enough to be treated analytically and yet are able to mimic the large diversity of dynamics of real glassy sys-tems.A well known example is the problem of a sin-gle particle driven by an external force f and subject to a one dimensional random force ?eld with Gaus-sian short range correlations.The term random force means that the correlator of the random potential U (x )is

(U (x )?U (y ))2≡K (x ?y )~?|x ?y |γ

(1)

and in Fourier space ?K

(q )=2π(1?cos qz )?

K (q ).We ?nd that there

are several regimes depending on how correlated the po-tential is.If correlations are short range (γ<0),we recover a ’viscous ?ow’(ohmic)regime where linear re-sponse V ~f holds for small f .If correlations grow with 0<γ<1we ?nd a new creep regime V ~exp(?1/f μ).The case γ=0corresponds to the transition between these two regimes and we ?nd a power law critical power

law V versus f dependence,reminiscent of the vortex glass transition behaviour[7].Finallyγ=1corresponds to Sinai’s case where V=0below a threshold force. This suggests a deep connection with the motion of elastic manifold in a random medium(such as vortex systems in type II superconductors).In these systems creep behaviour arises from the interplay of the elastic-ity and pinning potential[6]which both determine the creep barriers U b.The bare pinning potential is uncor-related but the elasticity of the manifold generates long range correlations in the e?ective potential U b that deter-mines the motion of the manifold.The role of elasticity as a tuning mecanism for correlations becomes transpar-ent upon noticing that the formation of the vortex glass is caused by a drastic change in elastic https://www.doczj.com/doc/ea16557196.html,ly, the onset of shear modulus at the freezing point devel-ops long range correlations in the vortex system[6].A phenomenological approach to describe a generic glass transition is to introduce a correlation lengthξG charac-terizing the spatial range of critical correlations,which diverges at the transition.The choice of K(x)on both sides of the transition is dictated by physical considera-tions.In the correlated phase(i.e glass phase)the natural choice is a Gaussian random potential with correlator of the form:

K(x?y)~?((|x?y|a)(2) The?rst term which dominates at large distance de-scribes long range correlations in the random potential and generalizes Sinai’s model.The second term describes the behaviour at the critical pointξG=∞.Indeed one hasγ=0and?K(q)~1/q at the transition and thus K(x)~?ln x.The form(2)is an interpolation resulting from the crossover between the critical?xed point and the?xed point describing the glass phase.In the uncorrelated phase correlations are short range and one chooses a correlator as?K(q)=1/

dt

=??U(x(t))+f+η(t)(3) with η(t)η(t′) =2Tδ(t?t′)and T is the temperature.The probability density P(x,t)and the current J(x,t) satisfy:

?P(x,t)

dt

=? +∞?∞dxx?J= +∞?∞dxJ(x,t)

= L0dx?J(x,t)(5)

where?J(x,t)=?T??P(x,t)+(f??U(x))?P(x,t).At long time?J(x,t)goes to a constant?J and the asymptotic velocity V is exactly given by V=?JL.To?nd?J for a ?xed L and disorder con?guration one must solve the stationarity equation:

T

??P(x)

T

(?U(x)+fx))does not,in general,satisfy the pe-riodic boundary conditions.Thus V can be found from the solution with non-zero current:

?P(x)=

?J

1?e(U(L)?U(0)?fL)/T

? x0dye(U(y)?U(x)+f(x?y))/T (7)?J and thus V follow from the normalization condition for?P.In the limit L→∞,imposing the restriction U(0)=U(L),unimportant for f>0,(7)simpli?es to:?P(x)=

?J

V

=

1

The average in (9)exists quite generally and is indepen-dent of the con?guration of the random potential,i.e the velocity is self-averaging.The physical interpretation of (9)in terms of Arrhenius waiting time is transparent.The average waiting time 1/V is a sum of Boltzman weights associated with the barriers the particle must overcome to move in the direction of the driving force.The highest barriers U (x +z )?U (x )with z >0,produce the largest waiting times.

The expression (9)reveals immediately several gen-eral features.At large f one has V ≈f .At small force f →0,the response will be linear only if the barriers saturate,i.e do not grow at large distance.If the potential is uncorrelated at large distances such that e (U (x +z )?U (x ))/T → e U/T e ?U/T when z →∞,then:

V ∝

D

e U/T e ?U/T

(10)

where D and D 0are the di?usion coe?cients in presence and in absence of disorder,respectively and the Einstein relation holds.When D ?D 0the V -f curve will show strong nonlinearity at intermediate scales where the tran-sition between low force and high force regime of motion occurs.

We now turn to a detailed study of gaussian disorder with correlator K (x ).Upon averaging over disorder (9yields:

1T ∞

0dx exp(?

fx

2T 2)(11)The choice of K (x )as in (2)gives rise to several regimes

of particle dynamics depending on the range of the cor-relations of the random potential.

Sinai’s case γ=1:For γ>1the integral in (11)di-verges and the velocity is zero.Sinai’s model corresponds to γ=1and appears as a marginal case where the in-tegral (11)diverges for f f th ,in agreement with previous results [15–17,19,20].The system with γ=1ex-hibits algebraic distributions of waiting times which gives rise to aging phenomena [20].Therefore Sinai’s model mimics essential aspects of the spin-glass behavior.In-terestingly,this V versus f dependence mimics also the dry friction phenomenon.

Creep motion 0<γ<1:In the intermediate case 0<γ<1one ?nds the ”creep”dynamics regime.De?n-ing the dynamical exponent z =2+(?/2T 2)and the characteristic force f c =(?/2T 2)1/γT/ξG one arrives at:T

f c z ?1

H (f/f c )

H (y )=

dv v z ?2exp(?yv +v γ)(12)Note that f c reduces to the threshold force f th when γ→

1.At γ<1the sharp threshold disappears but at f ?

f c the V versus f dependence shows strongly nonlinear behaviour with an essential singularity at small f .Usin

g the steepest descent method at f ?f c one ?nds:V =A T f c z ?1(

f

1?γ

exp(?(1?γ)(

γf c

1?γ

(13)

with A ~

Γ(z ?1)T 2+z

(14)

with z =2+(?/2T 2).resembling the power law

critical behaviour proposed at the vortex glass tran-sition.This transition separates the creep dynamics V ~exp(?const/f μ)in the vortex glass state from the ohmic behaviour V ∝f above the transition.Indeed one ?nds that the scaling function H (y )of (12)reproduces the correct scaling behaviour H (y )~y 1?z in the critical region y ?1which leads to (14)for T/a 2?f ?f c .Using (10)we ?nd the critical behaviour D ∝ξG 2?z .Since in the vortex system the voltage is proportional to the vortex velocity and force is proportional to applied current the obtained behaviour of D reporduces the crit-ical behaviour of the resistivity ρat the transition,ξG playing the role of the vortex glass critical length.

Ohmic behaviour γ≤0:For short-range correlations γ<0,

U (x )U (0)=?C (x ),

with C (0)=1and C (x )decays to zero on a length scale ξ.

1

T ∞

0dz exp(?

fz T 2(1?C (z )))(15)Two ohmic regimes,one at small force with V ∝e ??/T 2

f

and one at large force with V ∝f ,appear.At high tem-perature these two regimes match smootly.At low tem-perature there is a sharp crossover.A depinning temper-ature T p =

smooth crossover occurs at f c~T/ξ.For T<>f p.To estimate f p we use C(z)=exp(?(z/ξ)2) which leads to f p≈(T/ξ) ?/ξ.Note that f p does not depend on temperature and has thus a limit when T→0.At T→0the curve V versus f be-comes V=θ(f?f p)(f?f p).It is interesting to mention that this behaviour can be obtained correctly using the perturbation theory analogous to that used for calcula-tion of critical currents in type II superconductors[6]. Disorder induced corrections to the velocity is given by

δv/v=?ξvT?3(T

ξv )).Equatingδv/v≈1

we recover the above result for f p at low temperature T<>T p,δv/v never reaches1and thus f p does not exist.This analysis assume a?nite mean squared force<(?U)2>~f p2<∞,i.e that the random potential is smooth.If we choose instead C(z)=exp(?|z/ξ|)an exact calculation from(15)gives:

V=T

2T2

)fξ/T exp(??/2T)

whereγis the incomplete Gamma function.In that case the average force is in?nite and at T=0the particle remains pinned at any applied force.

The above model may apply directly to a string(di-rected polymer)of length L in d dimensions driven by its tip at z=0over point like impurities.An example is a ?ux line in a superconductor in presence of an external current J.Because of screening at small?elds the exter-nal Lorentz force of modulus f∝J is exerted only on the end of the line,over a length of orderλ.Let F(r)be the free energy corresponding to equilibrium positions r of the tip at z=0with the other end z=?L?xed at r=0 for large L.One can view the tip as a particle driven in the rough potential F(r)with

V

=

1

γδ?1(18) withν=1/(δ?1?γδ

Note added:After submission we received a preprint by S.Scheidl who also derived Eq.8.in a di?erent context.

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Open wide your little mouse But do not let them in 4. Gymbo Dance I have a little friend And Gymbo is his name oh G-Y-M-B-O G-Y-M-B-O G-Y-M-B-O And Gymbo is his name oh Gymbo the clown goes up and down up and down, up and down Gymbo the clown goes up and down All day long Gymbo the clown goes side to side side to side, side to side Gymbo the clown goes side to side All day long Gymbo the clown goes twist, twist, twist Twist twist twist Gymbo the clown goes twist, twist, twist Then he blows you a kiss

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16、收起心中的忧伤,抛开今天的抑郁,加添一份力量,今天必须洗去那悲伤! 17、你仿佛有一种魔力,那一刻我竟然无法言语。 18、其实你与昨日的我,活到今天变化甚多 19、我已背上一生苦困后悔与唏嘘,这眼里却此刻充满泪,竟然在这不知不觉的空虚,不想你别去。 20、太美的承诺因为太年轻! 21、等待我请等待我,靠近我再拥抱我,不要走请不要走,直到约定融化成笑颜,直到我看见生命的绝对。 22、愿这土地里,不分你我高低。缤纷色彩闪出的美丽,是因它没有,分开每种色彩。 23、终于你身影消失在人海尽头,才发现笑着哭最痛。 24、是缘是情是童真,还是意外。有泪有罪有付出,还有忍耐。 25、会感动我过一种生活,简单到没有奢侈的轻松。 26、你的爱就像彩虹,雨后的天空,绚烂却教人迷惑,蓝绿黄红。 27、不出声,不等于我满意现时,点解,你话你无事无事! 28、就请你给我多一点点时间,再多一点点问候,不要一切都带走。 29、你能推我下悬崖,我能学会飞行。 30、白月光,心里某个地方,那么亮,却那么冰凉。 31、你爱充满诱惑,让我着迷无法自拔的难过,而你却不愿意

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Little Bee Little bee, little bee 小蜜蜂小蜜蜂,Round round round 飞飞飞。 Little bee, little bee 小蜜蜂小蜜蜂,Sound sound sound 嗡嗡嗡。Bzzzzzzzzzz 嗡…… bee round sound 1. bee: 蜜蜂 little bee: 小蜜蜂 2. round: 旋转,环绕,兜圈子 3. sound: 发出声响 Open,shut Open, shut. Open, shut, 张、合、张、合, Give a little clap. 啪啪啪啪拍拍手。 Creep, creep, creep, creep, 爬、爬、爬、爬 Give a little flap. 啪啦啪啦飞得快。 open shut clap creep flap 1. open: 开 2. shut: 合拢(打开着的东西) 3. clap: n.拍手,拍手声v.鼓掌,轻敲 give a little clap: 拍拍手 4.creep: 慢慢地、悄悄地或偷偷地移动(尤指弯着腰走) 5. flap: n.拍打,拍打声,轻击 v.(使某物)上下或左右移动、摆动、摇动等(通常发出声响) give a little flap: 让它左右移动,就是飞起来 十个小手指 one little, two little, three little fingers 小小手指,一二三 four little, five little, six little fingers 小小手指,四五六 seven little, eight little, nine little fingers 小小手指,七八九 ten fingers on my hands 十根手指,是一家 three little fingers six little fingers nine little fingers ten fingers on my hands 1.little 小的;比较小的 2.finger 手指 3.hand 手 ten fingers on my hands 十根手指,是一家 the chimney Here is the chimney. 一个烟囱, Here is the top. 一个盖儿, Open the lid, 揭开这个盖儿, out Santa will pop. 圣诞老人冒出来! chimney lid Santa pop 1. chimney: 烟囱,烟筒 例句:Here is the chimney. 这是一个烟囱。 2. top: 盖子 例句: Here is the top. 这是一个盖子。 3. lid: 盖,盖子 4. pop: 突然从某物中出来,蹦出 Jack and Jill Jack and Jill went up the hill 杰克和吉尔, to fetch a pail of water 上山去打水。 Jack fell down 杰克滑倒了, and broke his crown 脑袋摔着了。 and Jill came tumbling after 吉尔跟着滑倒了。 hill pail a pail of water 1. hill: 小山,斜坡 2. fetch: (去)拿来 pail: 桶 a pail of water: 一桶水 例句:Jack and Jill went up the hill to fetch a pail of water. 杰克和吉尔上山取了一桶水。 3. crown: 敲(某人的)脑壳 broke his crown: 敲到了他的脑袋 4. tumble: 使摔倒,摔倒 come after: 跟着来,跟在后面 例句:Jill came tumbling after.吉尔跟着摔倒了。 two little black birds two little black birds,sitting on a hill 两只小黑鸟,坐在小山上 one named Jack,one named Jill一只叫杰克,一只叫吉尔 fly away Jack ,fly away Jill杰克飞走了,吉尔飞走了 Jack come back,Jill come back 杰克飞回来,

中国国歌的歌词

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Big Bang歌词

Big Bang - Number 1 Yeah~ Are you ready for the show~!!! I?ll be ready in an hour, jump in the shower Crisp and clean now I got the power Blasting music from my speakers T-shirts fresh, brand new sneakers Ready to flow, ready to go, Ready for the spot light, ready for the show Let me tell you something that you already know I?m a hardworking man and I work for my fans. Girl, I love your style, love your smile Wish that you could be Only mine, be only mine (fa?sho) I can?t let it go, I don?t kn ow What you?re doin? to me (yeah) You?re so fine (yeah uh huh), oh you?re so fine (let?s go) Gettin? hot in the club, I can see they want some more (I will give you more; I?m your number one) Once I get up I will rock, never stop, you can be sure (Yeah you can be sure; I?m your number one) I, (uh) you know I (yes) you know I(yo) I?m your number one. (I?m your number one) Crazy hot, mad party Shorty drop it low for me You can keep me company Your look sweet smell like honey I need a girl who is in it for me. Not for the money, not for the fame, Not for the glory, not for the name. It ain?t easy cause all they just sayin' is… “Boy I love your style, I love your smile Wish that you could be Only mine be only mine (fa?sho) I can?t let it go, I don?t know What you?re doin? to me You?re so fine, ooh you?re so fine” Gettin? hot in the club, I can see they want some more~ (I will give you more; I?m your number one) Once I get up I will rock, never stop, you can be sure~ (Yeah you can be s ure; I?m your number one) I, (you know I) you know I, (yeah you know I) you know I I?m you?re number one We jump, jump, jump to the ceiling (everybody in the place c?mon now) We jump, jump, jump what a feeling, feeling~ We jump, jump, jump to the ceiling, ceiling (once again BIGBANG c?mon) We jump, jump, jump, what a feeling, feeling~ Gettin? hot in the club yeah I can see they want some more~ you want some more (I will give you more I give you more ; I?m your number one) Once I get up I will rock rock rock rock never stop, you can be sure~ you can be sure (Yeah you can be sure; I?m your number one) Gettin? hot in the club, I can see they want some more~ (oh its getting hot in here~) (I will give you more; I?m your number one) Once I get up I will rock, never stop, you can be sure~ (Yeah you can be sure; I?m your number one) I, (you know I) you know I, (yeah you know I) you know I I?m you?re number one (I?m.your.number.one) Make love I never knew I?d find a love so true | This one right here, is just for you | Remember that One day | I held your hands then I kissed your lips then I told you | Our love was meant to be and always will forever | Give me that happiness I get from you just being there |

歌词说说大全

歌词说说大全 [标签:栏目] ,歌词说说大全 1、我会很快回来继续我们未完的天堂。 2、风卷过的起点,有疲倦也有种新鲜。太舍不得昨天,就去完成一个更幸福的明天。 3、我和你都约好了,要再唱这首笑忘歌。 4、想得太仔细,累坏了情绪。 5、我试过看开,尽量没感慨。 6、逃避没有出口,信仰爱就有可能你会发光的,何时为爱而活。 7、你要相信我,再不用多久,我要你和我今生一起度过。 8、我感受的、思想的、会用歌唱出来。 9、思念不再风吹时飘了,能够死心是种解脱。 10、为何不牵我的手,同看海天成一色。 11、我只是无辜的人,很需要叹气声。 12、只留下一段岁月,让我无怨无悔,全心的付出。 13、让悲伤麻木,快乐也开始麻木。 14、靠得再近也是种亏欠,我不是你随随便可以敷衍。 15、一句问候,对我来说也太多。 16、是否对你承诺了太多,还是我原本给的就不够。 17、花的心藏在蕊中,空把花期都错过。 18、我还没清醒,所以把自己关在房里。 19、愿这土地里,不分你我高低。缤纷色彩闪出的美丽,是因它没有,分开每种色彩。 20、告诉我你等待的是我,告诉我你不要再错过。 21、如果你身边找不到酒,把自己的影子饮用。如果你觉得有点词穷,让四只眼睛来沟通。 22、我们曾经那么精彩,我们曾经那么期待,最后你把回忆还我要我好好过。 23、眼泪咸哭到眼泪不咸,过一天痛一天。

24、能不能不要说,你想要的是什么,能不能就爱我。 25、你闪烁的眼眸,仿佛有些话始终无法说出口。 26、爱是一种天分,还是一种天真,我不多想我不多问。 27、你能推我下悬崖,我能学会飞行。 28、就让静夜吐心事,别让旧日创作牵绊着。 29、喜欢你,那双眼动人,笑声更迷人,愿再可,轻抚你,那可爱面容,挽手说梦话,像昨天,你共我。 30、不管身边始终不停有冷笑侵袭,你有你去干不会怕。 31、就算偶尔透露,你的不安和放纵,我总是相信你。 32、等待我请等待我,靠近我再拥抱我,不要走请不要走,直到约定融化成笑颜,直到我看见生命的绝对。 33、只为这一场命中的相遇,用我每一个呼吸去爱你。 34、爱你那么用力,却好像一场闹剧。 35、提着昨日种种千辛万苦,向明天换一些美满和幸福。 36、让你幸福是我一生在乎的事。 37、挣扎于风雨中已习惯,望能造个梦;失意总锻炼我,奋力去寻自我路。 38、冲出他朝崎岖道上,哪怕会退倒;试问谁人曾会考虑,过去与今天。 39、其实你与昨日的我,活到今天变化甚多 40、自始至终只能为你感动,和你相拥风中泪眼朦胧。 41、冷雨冷风锁着你心若是为了这便叹息垂头寻觅你的的影。 42、心中一把痴痴狂狂的剑,梦中朝朝暮暮的脸,最怕你看见我心里的剑,最怕把痴狂停在你眉尖。 43、多少泪还有多少的盼望,多少人变成紧闭门窗孤独的国王。 44、一双只懂哭的眼,落泪又再落泪。 45、梦不会实现了,我应该要醒了。 46、爱你够不够多,对你够不够好,可以要求不要不在乎。 47、你爱充满**,让我着迷无法自拔的难过,而你却不愿意施舍。 48、有些人没想像中的完美到没所谓。 49、握你的温柔,散落在我心中的是错过。我需要寂寞来抚摸,雨季中百花

whistle歌词

Can you blow my whistle baby, whistle baby(你能吹出我这样的口哨吗宝贝,口哨宝贝)Let me know(让我知道) Girl I'm gonna show you how to do it(女孩我这就要去告诉你怎么做) And we start real slow(然后我们慢慢开始) You just put your lips together(你只要把双唇合拢) And you come real close(然后你就能发出类似的(声音)) Can you blow my whistle baby, whistle baby(你能吹出我这样的口哨吗宝贝,口哨宝贝)Here we go(我们一起开始吧) I'm betting you like bebop(我猜你是喜欢比波普音乐的) And i'm betting you love creep mode(而且我猜你也喜欢令人惊悚的调式) And i'm betting you like girls that give love to girls(而且我猜你会喜欢关爱同性的女孩)And stroke your little ego(轻抚你的小小自我) I bet i'm guilty your honor(我猜你的荣誉令我感到内疚) But that's how we live in my genre(但这就是我们生活中的风格) When in hell I pay rottweiler(该死我到底该什么时候该付洛威纳犬的价钱) There's only one flo, and one rida(这儿只有一个Flo先生,一个Rida先生) I'm a damn shame(该死我真够惭愧) Order more champagne, pull it down hellstream(再点些香槟酒,倒下去) Tryna put it on ya(试着把它放在你那里) Bet your lips spin back around corner(我猜你角落边上的你会动动嘴巴) Slow it down baby take a little longer(慢一点宝贝(我希望你再)延长些时间) Can you blow my whistle baby, whistle baby(你能吹出我这样的口哨吗宝贝,口哨宝贝)Let me know(让我知道) Girl I'm gonna show you how to do it(女孩我这就要去告诉你怎么做) And we start real slow(然后我们慢慢开始) You just put your lips together(你只要把双唇合拢) And you come real close(然后你就能发出类似的(声音)) Can you blow my whistle baby, whistle baby(你能吹出我这样的口哨吗宝贝,口哨宝贝)Here we go(我们一起开始吧) Whistle baby, whistle baby,(口哨宝贝,口哨宝贝) Whistle baby, whistle baby(口哨宝贝,口哨宝贝) It's like everywhere I go(就像在我去过的所有地方一样) My whistle ready to blow(我随时都准备吹口哨) Shorty don't leave a note(这美女没留下什么便条) She can get any by the low(不过她轻易就能得到些) Permission not approved(这种允许可不被认可) It's okay, it's under control(这样就好,在我的控制之下) Show me soprano, cause girl you can handle(给我秀秀女高音,因为女孩你能搞定它)Baby we start snagging, you come in part clothes(宝贝我们开始消除阻碍,你让些新服饰登场)Girl i'm losing wing, my bucatti the same road(女孩我丢了翅膀,我的布拉迪跑车在同一条路上) Show me your perfect pitch,(向我展示出你最完美的音调) You got it my banjo(你已学会弹我的班卓琴) Talented with your lips, like you blew out candles(你的双唇天赋异禀就像你在吹蜡烛时一样)

中国歌词

[标签:标题] 篇一:中国梦歌词 中国梦- 陈思思 你在倾听我在倾听 一个声音在历史穿行你在追寻我在追寻一个夙愿让民族振奋啊这就是你的梦这就是我的梦这就是我们的中国梦中国梦啊文明梦中国梦啊和谐梦中国梦啊文明梦中国梦啊和谐梦沿着梦的方向触摸幸福我们走向新的征程 你在倾听我在倾听 一个声音在历史穿行你在追寻我在追寻一个夙愿让民族振奋啊这就是你的梦这就是我的梦这就是我们的中国梦中国梦啊强国梦中国梦啊富民梦中国梦啊强国梦中国梦啊富民梦 跟着梦的引领脚踏实地 我们走向伟大复兴中国梦啊强国梦 中国梦啊富民梦 中国梦啊强国梦 中国梦啊富民梦 跟着梦的引领脚踏实地 我们走向伟大复兴 - 篇二:我们的中国梦歌词 我们的中国梦 作词:晓岭 作曲:孟庆云 (合)啊你的梦我的梦梦的翅膀在飞翔 啊母亲梦儿女梦梦的翅膀在歌唱 (独)风儿送来春的气息让我与梦不期而遇 一滴露珠晶晶落下一双翅膀翩翩飞起 (合)寻一个幸福梦哪怕千里万里 飞过雪穿过雨我知道了新天地 薪火相传生生不息生生不息 啊你的梦我的梦梦的翅膀在飞翔 啊母亲梦儿女梦梦的翅膀在歌唱 (独)汗水染得山青水绿歌声引来花香鸟语 自豪的笑容多么甜蜜自信的道路开创奇迹 (合)寻到了幸福梦就在情里爱里 手相牵心相聚我看到了新天地 更加宽广更加美丽更加美丽更加美丽 毛委员和我们在一起 作曲:颂刚、春森、向义 作词:山樵、永立 红米饭那个南瓜汤哟咳罗咳,

挖野菜那个也当粮罗咳罗咳, 毛委员和我们在一起罗咳罗咳, 咳!餐餐味道香,味道香咳罗咳。 (二重唱)毛委员和我们在一起罗咳,餐餐味道香,味道香咳罗咳。 干稻草那个软又黄哟咳罗咳, 金丝被那个盖身上罗咳罗咳, 毛委员和我们在一起罗咳罗咳, 咳!心里暖洋洋,暖洋洋咳罗咳。 (二重唱)毛委员和我们在一起罗咳,心里暖洋洋,暖洋洋咳罗咳。 穿草鞋那个背土枪哟咳罗咳, 反围剿那个斗志旺罗咳罗咳, 毛委员和我们在一起罗咳罗咳, 咳!天天打胜仗,打胜仗,打胜仗。 (二重唱)毛委员和我们在一起罗咳,天天打胜仗,打胜仗,打胜仗。 篇三:共筑中国梦歌词 歌曲名称:共筑中国梦(2016年元旦教师大合唱)雄伟是山的梦宽阔是海的梦蔚蓝是天的梦幸福是百姓梦鲜花是春天的梦翱翔是雄鹰的梦远航是帆的梦强盛是中国梦满怀豪情领略浩荡的风踏平坎坷我们荣辱与共实现梦想拥抱天边彩虹我们昂首再启程共筑中国梦 雄伟是山的梦宽阔是海的梦蔚蓝是天的梦幸福是百姓梦鲜花是春天的梦翱翔是雄鹰的梦远航是帆的梦强盛是中国梦 满怀豪情领略浩荡的风踏平坎坷我们荣辱与共实现梦想拥抱天边彩虹我们昂首再启程共筑中国梦 满怀豪情领略浩荡的风踏平坎坷我们荣辱与共实现梦想拥抱天边彩虹我们昂首再启程共筑中国梦 共筑梦

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