Peer Assessment Essay Example | Topics and Well Written Essays - 1750 words

Peer Assessment - Essay Example My experience as a peer assessor was an eye opener. For the first time, I felt like I was not the one being reviewed, but I was reviewing other students' work. This gave me a sense of pride and courage and it also enabled me to see the big picture. In marking my classmate's papers, I no longer saw myself as a victim of marking but rather a victory. The peer assessment gave me an insight of one of the functions of our tutors, which is to assess the students' academic performance.   Our peer assessment was based on our assessment tests for all the units that we sat in the semester. The move was aimed at getting us to interact with each other while improving our leadership skills (Cottrell 2010). For the first time, my classmates and I felt some sense of responsibility for our education. It dawned on us that our education depends on us and that we are all equally talented when given a chance to review our peer's work. The assessment came as an encouragement to the not-so-good students that they can be trusted to assess even the brightest students in our class. Every student was assigned a paper to mark, and the tutor would guide us through the marking of the papers. The instructors used this opportunity to go through the questions with us, in an attempt to revise the paper. The teacher would guide us through, reading the questions aloud, and one after the other. He would then ask a classmate to provide the correct answer, and we would have a brief discussion on each issue.

Middle East Politics Essay Example | Topics and Well Written Essays - 1000 words - 1

Middle East Politics - Essay Example The main goal of this Anglo-American influence is to gain power and control on Middle East which is mainly due to their interest in the vast oil reserves in the region as well as western economic dependence. However, before the discovery of oil reserves in the region; Middle East was targeted by the western powers on the basis of religion (due to the presence different religions such as Judaism, Islam and Christianity in Middle East) and their interest in natural arable land. In the past, western powers had different motives behind this control but in modern times their main interest lies in those vast reserves of oil that has made this region attractive for the western super powers. As a result, these western forces are actively supporting the state of Israel due to their interest in oil reserves and to make Israel as their â€Å"closest ally† in the region. Due to their interest in gaining control upon Middle East; these western powers have played an important role in trigge ring this conflict by funding Israel though military aid and by supporting Israel in various international platforms. This conflict between Israel and Palestine revolve around different key issues between the two states such as control of Jerusalem, borders, water rights, security, violence against each other and Israel’s settlement in the West Bank. More than a dispute between two states; this issue is considered as a war between Arabs and Zionism by the Middle East. These Zionists represented the small Jewish population which was in search of settling down in a Jewish state. The increased immigration of Jews in Palestine triggered the conflict to grow more severe. This raised the tension between the Jews and the Arab population. In 1947, UN intervention gave an opportunity to Zionists to maintain their hold on 55% of the Palestine to the Jews. It was an irony to see that this group is consisted of 30% of the population with a 7% land control. It is also worth mentioning

The Worlds best ever performance Essay Example for Free

The Worlds best ever performance Essay When he got back to London he calmed himself and traveled back to Glasgow the next morning. Here he waited until Sven phoned him and announced the date of the next England match. He also told Douglas that the player who shouted at him was drunk and didnt know what he was saying.  Weeks later Douglas next match was only a few days away. He was hardened by his abuse and even more determined to play well in this match. When he finally jogged out onto the pitch the mixture of cheers and boos pumped him up to his best performance. On the pitch, Douglas was everywhere but as the match continued it became much like the next. He only got the ball when he managed to intercept his own teams pass and in his state of determination he knocked over an opposing player who was trying to tackle him. He was given a yellow card. The opposing team took a free kick. After the match Douglas headed out of the back entrance of the ground hoping to avoid angry hooligans but there were still plenty there, what he thought looked like thousands of people.  They were shouting comments, You Scottish pillock We hate you You suck Youre rubbish Were not goin to listen to your excuses even wit your crappy Scottish accent. The people shouted, Who do you think you are playing for us?  Later that day Douglas went into negotiations with the British Football Association. He wanted to know what they were going to do about the hooligans and players giving him abuse. He was very angry. What he was told by the BFA wasnt a great help either. They had agreed in a unanimous decision that Douglas should leave the team. They told him that it was because during his first two games he hadnt contributed to the final result. They told him he had hindered the team. At this comment Douglas went crazy, he tipped up his desk and rushed from the building so fast that a glass fell from another table.  During the next year of qualifying for the Europeans, England had numerous injuries. Some of the better known players were out, including Beckham, Owen and Cole. England needed some good new players. With only one week to go before the Europeans began the BFA phoned Douglas and said, We need your help Doug. It was Sven. Yu du? Realli. I wuldn hve guessed tha. Said Douglas, who was still hurt about his first two matches for England.  Douglas spent about half the weeks discussing terms and when it was finally settled he was flown down to London in a private Leah Jet.  He arrived in the stadium and boldly walked through a mass of confused supporters. They had not expected to see him back and had not been told by the press. Douglas was very confident and had a very good feeling about this game. The whistle blew and the game began. England played solidly and Poland, whom they had beaten in the first round of qualifying, did as well. However, the final score was England seventeen, Poland nil. Out of the seventeen goals scored Douglas had scored fifteen. This was the most goals scored at International level by any one player in any one match. It was a new World Record.  After this match, Douglas watched The News something which he had refused to do ever since his earlier experience for England. The same reporter as that time said in a bewildered voice, The Worlds best ever performance by a truly outstanding player. The other reporter then said, Yes it was. Literally. That match will be played on international television for centuries to come. Compared to the Scots last two England games it was more than jus beating a World record it was like beating twenty. This will open so many doors for McDonald and its a good present for his twenty-forth Birthday last week.  AS Douglas grew older he wrote a book on his experiences and discrimination. It became a best-seller and now hes a World record holder in Football and Literacy.

First-principles Study of Spin Transport in Si-C Nanotube

First-principles Study of Spin Transport in Si-C Nanotube First-principles study of spin transport in Si-C nanotube with ferromagnetic contacts Surendra Jalu Abstract  Ã¢â‚¬â€ We perform first-principles calculations of spin-dependent quantum transport in a two-probe device, viz. Fe-SiCNT-Fe device in which (8,0) Si-C nanotube is sandwiched between two Fe electrodes. Substantial tunnel magnetoresistance and perfect spin filtration effect are obtained. The zero bias tunnel magnetoresistance is found to be several hundred percent, it reduces monotonically till the bias voltage 0.4 V, sees marginal increase at the bias of 0.6 V, and eventually goes to nearly zero after the bias voltage of about 1 V. The spin injection factor is 100% at the zero bias, it reduces sharply to 57% at the bias of 0.4 V, and remains reasonably high, in the range of 60%-75%, after the bias voltage of 0.6 V when the magnetic configurations of two electrodes are parallel. The spin-dependent non-equilibrium transport features can be understood by analyzing microscopic details of the transmission coeà ¯Ã‚ ¬Ã†â€™cients. Keywords — First-principles; Tunnel magnetoresistance(TMR); Spin injection; One-dimensional; Spin filter I. Introduction Si-C crystals have unique properties, including thermal stability, chemical inertness, high thermal conductivity, and others. These properties make Si-C materials an appropriate candidate for fabricating electronic devices operating in high power, high temperature environments. Recently synthesized Si-C nanometer materials, such as nanorods, nanowires and nanotubes, have attracted tremendous interest (1-4). These materials obviously broadened the application range of the Si-C crystals, especially in fabricating nanometer gas sensors, electronic devices, field emitters and other novel devices. Silicon carbide nanotubes have a great potential for application in chemical and biological sensors (Taguchia et al 2005a; Xie et al 2007). Recently, scientists have suggested to make silicon carbide nanotubes (SiCNTs) as a possible alternative to carbon nanotubes (CNTs) for field emitting applications (Taguchia et al 2005b; Alfieri and Kimoto 2010), which has boosted the interest for SiCNTs and several studies on the electronic properties of SiCNTs can be found in the literature (Mavrandonakis et al 2003; Mpourmpakis et al 2006; Larina et al 2007; Muralidharan et al 2007; Wu and Guo 2007; Lakshmi et al 2008; Moradian et al 2008; Raidongia et al 2008; Voggu et al 2008; Wu et al 2008; Manna and Pati 2010; Zheng et al 2010). It is well known that CNTs undergo a semiconductor to metal transition (SMT) (Ren et al 2009) or metal to semiconductor transition (MST) (Lu et al 2003) when deformed. Therefore, it is of interest to understand how the semiconducting (8,0) SiCNT would behave when i t is brought in contact with ferromagnetic electrodes. On account of important applications in magnetoresistive random access memory [1], programmable logic elements [2] and magnetic sensors, the giant magnetoresistance (GMR) and tunnel magnetoresistance (TMR) effects in systems with spin-polarized transport are at the heart of spintronics [3] and attract many theoretical and experimental investigations. A basic magnetic tunnel junction (MTJ) device consists of tunnel barrier separating two ferromagnetic (FM) layers which play the role of device leads. During a tunneling process, the spin-up and spin-down electrons from the metal layers traverse the nonmagnetic tunnel barrier with different Fermi wave function due to electronic structure of the ferromagnetic material. The electrical resistance of MTJ is therefore sensitive to the relative orientation of the magnetic configuration of the electrodes, resulting to a TMR [4]. Hence, the MTJs behave as spin valves [4–8]. It is possible to control the orientation of magnetic moments by imposing an external magnetic field in experiments [9,10]. It is important to note that, MgO-based MTJ has progressed at a rapid pace in recent years and produced the highest measured TMR at room temperature. When the electrodes and the tunnel barrier are all one-dimensional (1D) materials such as nanowires or nanotubes, it is experimentally feasible to achieve MTJ at the 1D scale. It is worth mentioning that Wang et al. [12] construct a 1D TMJ using Fe-doped carbon nanotubes and theoretically investigate its spin-dependent transport properties. What is a pity that, the zero bias magnetoresistance ratio is only ∠¼ 40%, which may restrict the spintronics applications in nanodevices where the large magnetoresistance ratio is desirable. Here, we theoretically investigate the spin-polarized transport of a 1D MTJ constructed by (8,0) SiCNT in contact with FM(Fe) electrodes. It is observed that (8,0) SiCNTs are semiconducting and we believe that it can be used as a tunnel barrier for 1D or molecular-scaled MTJ. In our work, We have chosen (8,0) SiCNT as the tunnel barrier and two semi-infinite FM materials, namely Fe, as electrodes. Significant TMR and perfect spin filtration effect are obt ained according to the first-principles calculations of spin-polarized quantum transport by adopting non-equilibrium Green’s function method combined with density-functional theory. TMR has already led to the construction of the present generation of magnetic data storage devices. However, in order to reach storage densities of the order of Terabit/inch2, a substantial down-scaling of the read/write devices is extensively expected. Such 1D MTJ and spin filter with diameter less than 1 nm may realize the storage densities of the order of Terabit/inch2 and hold promise for extensive spintronics applications of nanodevices. II. Model and method Our investigation is based on a recently developed self-consistent first-principles technique which combines the Keldysh non-equilibrium Green’s-function formalism (NEGF) with a self-consistent density-functional theory (DFT). The package we use is the Atomistix Toolkit [20], which incorporates the NEGF technique into the well tested SIESTA method [21] to realize the simulation of electrical or spin-polarized quantum transport in the molecular conductors under non-equilibrium situations. In the calculation, the local density approximation (LDA) in the form of the Perdew and Zunger [22] (perdew burke ernzerhof) exchange-correlation functional is used. Only valence electrons are self-consistently calculated, and the atomic cores are described by standard norm conserving pseudopotential [23]. The valence wave functions are expanded by the localized numerical (pseudo) atom orbitals [24]. The k-points sampling is 3, 3, and 200 in the x, y, and z direction, which has been proven to be enough to give the converged results. The convergence criterion for the Hamiltonian, charge density, and band-structure energy is 10-5 via the mixture of the Hamiltonian. The positions of C and Fe atoms at the interface of the device are relaxed until the force tolerance 0.05 eV/Ã… is achieved. The spin-current (spin-polarized charge current) is calculated [25] as I↑(↓) = e/h ∠« T↑(↓)(E, Vb) [F(E − ÃŽ ¼L) – F(E −  µR)] dE [R] Where F is the Fermi–Dirac distribution, ÃŽ ¼L and ÃŽ ¼R are the chemical potentials of left-electrode (L) and right-electrode (R) respectively, T↑(↓)(E, Vb) is the transmission coeà ¯Ã‚ ¬Ã†â€™cient for spin channel ( ↑ , ↓ ) at the energy E and bias voltage Vb. While building SiCNT, it is utterly important to use optimum bond-length between Si and C atoms to obtain correct results which in our case, as mentioned in various literatures, is 1.78 Ã…. We couldn’t find the optimum bond-length between C and Fe atoms in literature but we were able to optimize a geometry that consisted of only a few atoms of Fe and C and this way we found the optimum bond-length between Fe and C atoms to be 2.04 Ã… (Fig. 4 (b)). The whole system (Fig. R) is divided into three parts from left to right in practical theoretical simulations: the left electrode, the central scattering region, and the right electrode. The left electrode and right electrode are exactly the same and are made of Fe atoms. Si-C nanotube acts as central scattering region between two electrodes. The whole structure contains 328 atoms (192 Fe, 72 C, 64 Si). 4 (a) 4 (b) Fig. 4(a) Fe-C bond-lengths in non-optimized geometry 4(b) Fe-C bond lengths in optimized geometry Fig. 4(c) Fe-SiCNT-Fe device III. results and discussions Fig. 2(a) and (b) plot the current–voltage (I–V) characteristics for the parallel magnetization configuration (PC) and the antiparallel magnetization configuration (APC) of the two electrodes, respectively. In the case of PC, the spin-up current (I↑) are always much larger than the spin-up current (I↓). The I↑ increases steeply with bias voltage especially after the bias of 0.8 V while on the other hand I↓ is almost negligibly small compared to I↑ at almost all bias voltages. The total equilibrium conductance of 0.0022G0 is found at zero bias, where G0 is the conductance quanta, G0 = 2e2/h. In the case of APC, I↑ and I↓ have almost the same values at all bias voltages. The total equilibrium conductance of 0.0095G0 is found at zero bias. From the I–V curves, we infer a TMR ratio using the common definition: TMR = (IAPC − IPC)/IAPC, where IPC and IAPC are the total currents in PC and APC, respectively. At Vb = 0 when all currents vanish, we calculate TMR using equilibrium conductance. Fig. 2(c) shows the TMR, where the RTMR ∠¼ 322% at zero bias is obtained, which indicate in the perfect tunneling magnetoresistance effect. It sharply decreases to ~ 80% at the bias voltage of 0.4 V, sees slight increase at the bias voltage of 0.6 V and gets reduced to almost zero after the bias voltage of 1 V. The TMR decrease with bias voltages because IPC increases at higher rate with bias voltages than IAPC. It is possible for TMR to assume negative value but in our case no such behavior is observed. The device structure presented here indeed has substantial TMR and could be utilized for spintronics applications. The spin-injection factor ÃŽ · which is defined by spin currents: ÃŽ · = mod(I↑ I↓) / (I↑ + I↓) are plotted in Fig. 2(d). At the bias voltage of 0.0 V, the current is 0 A and hence we use the equilibrium conductance represent current. For the case of PC, ÃŽ · is 99% at the zero bias, it monotonically reduces to 57% at the bias voltage of 0.4 and it increases and remains fairly within large values once the bias voltage goes beyond 0.4 V. The spin-injection factor ÃŽ · is as large as ~73% at the bias of 1.2 V and may even improve at higher bias voltages. For the case of APC, the ÃŽ · is meager ~49% at the zero bias. It’s dramatic that it reaches ~85% at the bias voltage of 0.2 V but then it keeps reducing with increase in bias voltages and attains very negligible values at the bias of about 1 V to 1.2 V. From Fig.R it is observed that in the case of PC the spin filtration effect manifests itself very clearly when the bias is above 0.4 V while in the case of APC no such effect is seen. The source of this behavior maybe originates from the quantum size effect which results in the quantized subbands in the cross section of 1D electrode. Detailed analysis is in the below. Spin injection into semiconductors has been measured experimentally using the optical techniques [26,27]. Such 1D TMJ contr olled spin injection into semiconductors should occur in devices that are smaller than a spin relaxation length in extent and have resistance that is limited by the insulating BNNT. The voltage dependent of spin current, TMR ratio and spin-injection factor can be understood from the behavior of the transmission coeà ¯Ã‚ ¬Ã†â€™cients [ T (E, Vb) ] , since the current is essentially given by the energy integral of the T (E, Vb) over the bias window [see Eq. (1)]. The T (E, Vb) for several bias are shown in Fig. 3, where the (a) and (b) are spin-up and spin- down channel of PC setup respectively and the (c) and (d) are spin-up and spin-down channel of APC setup respectively. For both PC and APC setup, these bias-depended T(E,Vb) have several sharp peaks especially after the bias of 0.35 V, due to quantized subbands in the cross section of the 1D electrodes, already mentioned above. The spin up channel contribute to the T(E,Vb) above the Fermi level and spin-down channel contribute both above and below the Fermi level. Refer to the notation from molecular transport theory [28] we can deduce that the spin-up channel conductance is through the lowest unoccupied molecular orbital (LUMO) while the spin-down channel conductance is through both the highest occupied molecular orbital (HOMO) and LUMO of pristine (6,0) BNNT in scattering region. From Fig. 3(a), one can see that the T (E, Vb) shifts to high energy but roughly maintains its shape when bias increases. The T (E, Vb) are all almost absolutely inhibited in spin-up channels around Fermi level, while in the spin-down channel the T (E, Vb) is smooth and several orders of magnitude larger than in spin-up channel around Fermi level. This is why the I↓ linearly increases while the I↑ is inhibited under the bias of 0.75 V, already discussed above for Fig. 2(a). As the bias increases, the electrochemical potential in the left electrode (ÃŽ ¼L) is shifted down, and that in the right electrode (ÃŽ ¼R) is shifted up. Hence, the bands in the two electrodes are shifted correspondingly [29–32]. When the bias increase beyond 0.75 V, a little resonance states A1 are induced around Fermi level showed in Fig. 3(a) for the bias of 0.75, 0.95 and 1.15 V, which originate from the alignment of the LUMO of left electrode with the HOMO of right electrode in spin-up channel because the bands in the two electrodes are shifted. These resonance states significantly enhance as bias increasing, which result in the rapid increase about I↑ after the bias of 0.75 V. Consequently, the rapid increase of I↑ also leads to the rapid decrease about ÃŽ · for PC setup after 0.75 V, already discussed above for Fig. 2(c). The bias dependent T (E, Vb) for APC setup are more complex than PC setup. From Fig. 3(c), one can see that the T (E, Vb) in spin-up channel roughly maintains its shape when bias increases. A little resonance states A2 below Fermi level, which presents for the bias of 0.00 and 0.15 V are removed after the bias of 0.15 V. As the bias increase, only a little resonance states above the Fermi level enter to the transport window (i.e., the part of transmission function in the bias window integrated to obtain the current) and contribute to the I↑, which result in very slow increase of the I↑. After the bias of 0.15 V, the T (E, Vb) shifts to larger energy and large resonance states are induced around Fermi level due to the alignment of spin-down states around Fermi level of left electrode with HOMO of right electrode in spin-down channel because the bands in the two electrodes are shifted. These induced resonance states continuously enhance as bias increase, which result in r apid increase of I↓. Eventually, the total current for APC setup exceed PC setup after the bias of 0.75 V, result in negative RTMR, already discussed above for Fig. 2(c). As mentioned above, the quantum size effect leads to the quantized subbands in the cross section of 1D electrode. Hence, there are two peaks in the induced resonance states around Fermi level after the bias of 0.35 V, showed in Fig. 3(d). When T (E, Vb) continuously shifts to higher energies, these two peaks pass the Fermi level one by one, which cause the oscillation about the spin-down conductance. Thus, the spin injection factor ÃŽ · is oscillating with bias in the APC setup. IV. conclusion We theoretically investigate the spin-polarized transport properties of V atoms doped (6,0) single-wall BNNT using non-equilibrium Green’s-function formalism with a self-consistent density- functional theory. The RTMR is as high as 789% at the bias of 0.05 V. It decays to zero and eventually to negative values when bias is increased. The ratio of spin injection is not below 99% until the bias of 0.55 V when the magnetic configurations of two electrodes are parallel. When the magnetic configurations of two electrodes are antiparallel, the ratio of spin injection oscillates with the bias. Our calculations indicate that it could design perfect 1D MTJs and spin filter using TMs doped BNNTs. The perfect TMR effect and spin filter effect are obtained. References The template will number citations consecutively within brackets [1]. The sentence punctuation follows the bracket [2]. Refer simply to the reference number, as in [3]—do not use â€Å"Ref. [3]† or â€Å"reference [3]† except at the beginning of a sentence: â€Å"Reference [3] was the first † Number footnotes separately in superscripts. Place the actual footnote at the bottom of the column in which it was cited. Do not put footnotes in the reference list. Use letters for table footnotes. Unless there are six authors or more give all authors’ names; do not use â€Å"et al.†. Papers that have not been published, even if they have been submitted for publication, should be cited as â€Å"unpublished† [4]. Papers that have been accepted for publication should be cited as â€Å"in press† [5]. Capitalize only the first word in a paper title, except for proper nouns and element symbols. For papers published in translation journals, please give the English citation first, followed by the original foreign-language citation [6]. G. Eason, B. Noble, and I.N. Sneddon, â€Å"On certain integrals of Lipschitz-Hankel type involving products of Bessel functions,† Phil. Trans. Roy. Soc. London, vol. A247, pp. 529-551, April 1955. (references) J. Clerk Maxwell, A Treatise on Electricity and Magnetism, 3rd ed., vol. 2. Oxford: Clarendon, 1892, pp.68-73. I.S. Jacobs and C.P. Bean, â€Å"Fine particles, thin films and exchange anisotropy,† in Magnetism, vol. III, G.T. Rado and H. Suhl, Eds. New York: Academic, 1963, pp. 271-350. K. Elissa, â€Å"Title of paper if known,† unpublished. R. Nicole, â€Å"Title of paper with only first word capitalized,† J. Name Stand. Abbrev., in press. Y. Yorozu, M. Hirano, K. Oka, and Y. Tagawa, â€Å"Electron spectroscopy studies on magneto-optical media and plastic substrate interface,† IEEE Transl. J. Magn. Japan, vol. 2, pp. 740-741, August 1987 [Digests 9th Annual Conf. Magnetics Japan, p. 301, 1982]. M. Young, The Technical Writer’s Handbook. Mill Valley, CA: University Science, 1989.

Ozzie Freedman Portrayed as a Hero Essay example -- essays research pa

Ozzie Freedman Portrayed as a Hero   Ã‚  Ã‚  Ã‚  Ã‚  A hero can be defined as one who inspires through manners and actions; who leads through personal example. Under this definition, the character Ozzie Freedman from Philip Roth’s â€Å"The Conversion of the Jews† (1959) can be classified as a hero. The sections of Discoveries: Fifty Stories of the Quest (Schechter & Semekis 1992): The Call, The Other, The Journey, Helpers and Guides, The Treasure, and Transformation, can be applied to the story about Ozzie to support it’s inclusion in this class, entitled â€Å"Myth of the Hero†.   Ã‚  Ã‚  Ã‚  Ã‚  The chapter on The Call describes that a hero may be â€Å"on the brink of a decisive change† (21) and they â€Å"perceive the danger of remaining where they are† (22). The hero must be â€Å"ready †¦ to leave [his] old, familiar [life] behind and move on to something new† (23). In â€Å"The Conversion of the Jews†, we see Ozzie questioning his faith and going against the Jewish teaching by believing that God could â€Å"let a woman have a baby without having intercourse† (384). He stood up to the rabbi in class and was prepared to defend his questioning and beliefs.   Ã‚  Ã‚  Ã‚  Ã‚  The Other is a character who embodies the exact opposite personality of the protagonist. According to Schechter & Semekis, the Other causes self-revelation in the protagonist, which his journey would not begin without. In Roth’s story, Itzie is Ozzie’s best friend, who does not question authority or his faith, quite the opposite of Ozzie. He gives Ozzie a hard time for always asking questions and speaking out in class. (‘â€Å"What do you open your mouth all the time for?†Ã¢â‚¬â„¢ (383)). Ozzie realizes he doesn’t want to be like Itzie and blindly accept the Jewish belief about Jesus. He defends his right to question something in order to seek validity, and says, ‘â€Å"Itz, I thought it over for a solid hour, and now I’m convinced God could do it.†Ã¢â‚¬â„¢   Ã‚  Ã‚  Ã‚  Ã‚  Discoveries describes The Journey as a portrayal of â€Å"how difficult the hero’s quest is† (8). In Roth’s story, Ozzie faces â€Å"external enemies, agents of conservatism or conformity that must be overcome† (Schechter & Semekis, 8). He is speaking out against the Jewish religion, saying that he believes God could impregnate a woman without her having intercourse. When he delivers this defiance to Rabbi Binder, he is... ...nbsp;  Ã‚  Ã‚  Ã‚  By applying the theory of the hero’s journey as found in Discoveries: Fifty Stories of the Quest and applying it to Roth’s â€Å"The Conversion of the Jews†, we see that the character Ozzie Freedman truly fits the title of a hero. Ozzie questions his religious beliefs and is not ashamed to bring forth his insight and seek answers and new ways of thinking. He winds up teaching his mentor a lesson in religion and sets out to have his message heard, despite the possibility of ridicule and even death. Once he realizes he has a different belief than the people of the Jewish religion, he understands his life will never be the same and that he cannot go back to the Jewish belief that God is not able to produce a child without intercourse. Ozzie gets his message across, that one should never be punished for his beliefs, and he is then born into a new day and a new life journey. Works Cited Roth, Philip. â€Å"The Conversion of the Jews.† Discoveries: Fifty Stories of the Quest. 2nd ed. Harold Schechter and Jonna Gormely Semekis. New York: Oxford, 1992. Schechter, Harold, and Jonna Gormely Semekis. Discoveries: Fifty Stories of the Quest. 2nd ed. New York: Oxford, 1992.

Psychological Profile of Holden Caulfield Essay -- The Catcher In Th

Psychological Profile of Holden Caulfield Part One: The patient is Holden Caulfield, a sixteen-year-old teenage boy. Caulfield's appearance is tall for his age and surprisingly has quite a few gray hairs at the age of sixteen. Holden comes from an upper-middle class family. His family has enough money to support Holden with many luxuries including skates and expensive suitcases. It appears that Mr. and Mrs. Caulfield aren?t there to talk, care, and be there for Holden, which seems to drive Holden away from his family. However, he has an intimate bond with his younger siblings, who embody innocence and youth. The death of his brother Allie has left a large scar on Holden. He has a cherished and intimate relationship with his young and innocent sister, Phoebe. Holden has been to many schools and has been kicked out of many schools. Holden is an intellectual teenager, who refuses to apply himself, and thus goes from school to school. Some of the important and affecting moments in Holden?s life are death of Allie, suicide of a close friend, D.B. ?selling out?, and his summer with Jane Gallagher. Allie, Holden?s younger brother died of leukemia recently and has caused stress upon the patient. Also witnessing the death of once close friend traumatized the patient. The fact that Holden?s friend committed suicide wearing some of his clothing, placed even more strain on the patient. Another factor surround Holden is his brother D.B. leaving him and his family to ?sell out to Hollywood? disturbed Holden. Lastly, the summer he had spent with a close and intimate friend, Jane Gallagher had added fuel to fire, which drove Mr. Caulfield to this institution and require professional help from our clinic. Part Two: The patient, Holden Caulfield, perceives himself a ?madman?. Holden proclaims he is a madman for his actions and thoughts. With the analysis of Holden Caulfield?s description of the weekend leading up to his enlistment of professional care for chronic depression, Holden reveals his thoughts on being convinced he was a madman. One incident from Holden?s description explicitly gives Holden?s view of himself. The incident in reference is his date with Sally Hayes. Holden proposed to Sally to run away to Massachusetts and live together away from the world. In actuality Holden could not tolerate Sally and her ?phoniness?, but he still made the sug... ...hem. Holden Caulfield is capable of recovery, but will require intense work and help. A timeline for his recovery could be anywhere from three months to as long three years. Currently, I believe it will take approximately six months for Holden to fully recover based on his interactions with the staff here at Bergen Pines. When asked by a psychoanalyst about applying himself in school next year, his response was, ?It?s such a stupid question, in my opinion. I mean how do you know what you?re going to do till you do it (Salinger 213). In this response, there are remnants of hostility and anger remaining him Holden, which would make me believe it would take a full year in order for him to recover. However, in Holden?s account it states, ?I sort of miss everybody I told about. Even old Stradlater and Ackley, for instance. I think I even miss that goddam Maurice? (Salinger 214). In this statement, it makes me believe that Holden is already working to return back on the path of sanity, because he lets go of the phony business and outright states he is beginning to miss his friends and the people he met. This is a sign that shows me he is bound to recover as soon as six months.

Part Five Chapter II

II ‘Brace yourself,' teased Howard Mollison at midday on Saturday. ‘Mum's about to post the results on the website. Want to wait and see it made public or shall I tell you now?' Miles turned away instinctively from Samantha, who was sitting opposite him at the island in the middle of the kitchen. They were having a last coffee before she and Libby set off for the station and the concert in London. With the handset pressed tightly to his ear, he said, ‘Go on.' ‘You won. Comfortably. Pretty much two to one over Wall.' Miles grinned at the kitchen door. ‘OK,' he said, keeping his voice as steady as he could. ‘Good to know.' ‘Hang on,' said Howard. ‘Mum wants a word.' ‘Well done, darling,' said Shirley gleefully. ‘Absolutely wonderful news. I knew you'd do it.' ‘Thanks, Mum,' said Miles. Those two words told Samantha everything, but she had resolved not to be scornful or sarcastic. Her band T-shirt was packed; she had had her hair done and she had bought new heels. She could hardly wait to leave. ‘Parish Councillor Mollison then, is it?' she said, when he had hung up. ‘That's right,' he said a little warily. ‘Congratulations,' she said. ‘It's going to be a real celebration tonight, then. I'm sorry I'm missing it, actually,' she lied, out of excitement at her imminent escape. Touched, Miles leaned forward and squeezed her hand. Libby appeared in the kitchen in tears. She was clutching her mobile in her hand. ‘What?' said Samantha, startled. ‘Please will you call Harriet's mum?' ‘Why?' ‘Please will you?' ‘But why, Libby?' ‘Because she wants to talk to you, because,' Libby wiped her eyes and nose on the back of her hand, ‘Harriet and I've had a big row. Please will you call her?' Samantha took the telephone through to the sitting room. She had only the haziest idea who this woman was. Since the girls had started at boarding school she had virtually no contact with their friends' parents. ‘I'm so desperately sorry to do this,' said Harriet's mother. ‘I told Harriet I'd speak to you, because I've been telling her it's not that Libby doesn't want her to go †¦ you know how close they are, and I hate seeing them like this †¦' Samantha checked her watch. They needed to leave in ten minutes at the latest. ‘Harriet's got it into her head that Libby had a spare ticket, but didn't want to take her. I've told her it's not true – you're taking the ticket because you don't want Libby going alone, aren't you?' ‘Well, naturally,' said Samantha, ‘she can't go alone.' ‘I knew it,' said the other woman. She sounded strangely triumphant. ‘And I absolutely understand your protectiveness, and I would never suggest it if I didn't think it would save you an awful lot of bother. It's just that the girls are so close – and Harriet's absolutely wild about this silly group – and I think, from what Libby's just told Harriet on the phone, that Libby's really desperate for her to go too. I totally understand why you want to keep an eye on Libby, but the thing is, my sister's taking her two girls, so there would be an adult there with them. I could drive Libby and Harriet up together this afternoon, we'd meet up with the others outside the stadium and we could all stay overnight at my sister's place. I absolutely guarantee that my sister or I will be with Libby at all times.' ‘Oh †¦ that's so kind. But my friend,' said Samantha, with a strange ringing in her ears, ‘is expecting us, you see †¦' ‘But if you still wanted to go and visit your friend †¦ all I'm saying is there's really no need for you to attend, is there, if somebody else is with the girls? †¦ And Harriet's absolutely desperate – really desperate – I wasn't going to get involved, but now it's putting a strain on their friendship †¦' Then, on a less gushing note, ‘We'd buy the ticket from you, of course.' There was nowhere to go, nowhere to hide. ‘Oh,' said Samantha. ‘Yes. I just thought it might be nice to go with her – ‘ ‘They'd much prefer to be with each other,' said Harriet's mother firmly. ‘And you won't have to crouch down and hide among all the little teenyboppers, ha ha – it's all right for my sister, she's only five foot two.'