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المبحث الخامس: بدايةالنظم عند نازك الملائكة

المبحث الخامس: بدايةالنظم عند نازك الملائكة
نظمت الشاعرۃ العراقیۃ نازک الملائکۃ قصیدتھا الأولی ’’الکولیرا‘‘ في عام 1947م وکان عمرھا آنذاک اثنین وعشرین عاماً، وكذا بدأت حرکۃ الشعر الحرعام 1947م، في العراق وزحفت ھذہ الحرکۃ حتی عمت وأحاطت بالوطن العربي کلہ . تقول رائدۃ الشعر الحر في قضایا الشعر المعاصر: ’’وکانت أول قصیدۃ حرۃ الوزن تنتشر قصیدتي المعنونۃ الکولیرا‘‘وھي من الوزرن المتدارک(الجنب) ۔
کانت نازک الملائکۃ شاعرۃ رائعۃ وحساسۃ جداً، صورت مشاعرھا وعبرت عن حزنھا بتعبیر صادق، وتکلّمت عن إخوانھا المرضی بداء ’’الکولیرا‘‘ في مصر، فکان ذلک سبباً في اکتشاف أسلوب جدید في الشعر الحدیث وھو ’’ الشعر الحر‘‘۔
في مطولتھا الشعریۃ ’’مأساۃ الحیاۃ‘‘ أخذت الشاعرۃ تبحث عن السعادۃ متسائلۃ إن کان لھا الوجود في ھذہ الدنیا الفانیۃ، فبحثت أولاً لدیٰ الأغنیاء لعل السعادۃ في قصورھم وحیاتھم المترفۃ الناعمۃ، ولکنھا وجدت الغني بأن لیس لہ القدرۃ علی أن یدفع وحشۃ القبر والأکفان بأحوالہ وثروتہ، ثم انتقلت إلی الرھبان والزاھدین فوجدت آثار الحرمان من اللّذات واضحۃ علی وجوھھم، ثم انتقلت إلی اللصوص والمجرمین فوجدت لدیھم القلق وعذاب الضمیر ولیس لدیهم راحۃ البال. فاتجھت نحو الریف، وھناك أیضاً لم تجد السعادۃ بل وجدت البؤس والفقر والعذاب، ووصفت حال الفلاحین في المناطق الباردۃ التي فیھا الثلوج وکیف ینتشر الجوع وتموت المواشي، ثم انتقلت من الریف إلی الشعر والشعراء، ولا نجد السعادۃ لدیھم، فاتجھت الی العشاق والمحبین لعلھم ذاقوا السعادۃ ولکن للأسف لا تجد فیھم السعادۃ وذلک لأن الشھوۃ الجنسیۃ تفوق الفکر العقلي والحب الشریف وتعاند طھارۃ الروح الإنساني، فانتھت رحلۃ الشاعرۃ بالخیبۃ حيث لم تجد لدیھم السعادۃ۔
وتطور أسلوب شعرھا في عام 1950 فأصبحت مواردھا الأدبیۃ أغزر ولم تکن راضیۃ عن (مأساۃ الحیاۃ) فقررت أن تعید نظمھا بصورۃ أجمل وبأسلوب جدید، فتطور ألفاظھا يختلف عن الألفاظ السابقۃ وأخذت تعدل ھذہ المطولۃ وتضع شطراً ھنا وھناک وبدأت التغیرات تطرأ علی القصیدۃ بشكل كامل دون أن تأخذ من المطولۃ الأولی لفظۃ واحدۃ، ثم...

دین کامل اور اختلاف: روح المعانی کی روشنی میں ایک تحقیقی جائزہ

The word "Ikhthilaf" refers to such an approach and way of conversation in which one scholar disagrees with another scholar. Islam being a perfect religion bars its followers from developing mutual conflicts. Islam has clearly stated that Muslim Ummah should not have differences on the basis of opinions in vivid injunctions. Such dissension has been placed nowhere in Islam. Disputes may only arise in case of secondary and vague injunctions. In such situations, each jurist considers himself as right. Such divergence, in the secondary issues based on argumentation and within the ambit of Qur’ān and Ḥadith, is not contemptible one but is the source of blessings due to the depth of knowledge of the jurists. Because of such conflicting opinions, jurisprudence and religious injunctions have the power of adaptability in accordance with the demands of the changing times. In the matters of jurisprudence, establishing consensus on the basis of argumentation must not lead to sectarianism, prejudice and hatred. True jurists have tried their level best to protect Muslim Ummah from sectarian disputes. Among such jurists we have Allama Alusī, the author of Tafsīr Rūḥ al Ma’ānī, as one big contributor. Tafsīr Rūḥ al Ma’ānī is the solid proof of his authentic and deep knowledge. It has a combination of reported sayings and exegesis of consents.

J/Ѱ Interaction With Light Mesons in Qcd-Improved Cornell Model for Tetraquarks

We have calculated the cross-sections for the processes ρJ/ψ → D0 ¯ D0, ρJ/ψ → D0 ¯ D0∗ or D0∗ ¯ D0, ρJ/ψ → D0∗ ¯ D0∗, D0 ¯ D0 → ρJ/ψ, D0∗ ¯ D0 or D0 ¯ D0∗ → ρJ/ψ and D0∗ ¯ D0∗ → ρJ/ψ using a QCD-motivated improvement to the usual sum of pairwise interaction model. This improvement is modelled in the literature by a gluonic field overlap factor f multiply ing off-diagonal elements of normalization, kinetic energy and potential energy matrices in the basis composed of different q¯ q clusterings of a two quarks two antiquarks system. We study the effect of this f factor in these meson-meson scatterings. Gaussian form of f i.e. (exp(−bskf∑i<j r2 ij)) is taken for computational convenience. The chosen value of the parameter kf is originated from numerical lattice QCD simulation. For a comparison, we also calculated the cross sections for f = 1 meaning the sum of pair-wise model limit. The Res onating group method has been used to make a maximum use of the wave function of a single cluster of a quark anti-quark pair. Kinetic energy and overlap matrices have been treated on the model of the potential matrix in the gluonic basis. Here quadratic wave functions are taken by fitting the parameters in such a way that we get maximum overlap of meson quadratic and Cornell wave functions. In order to decouple the coupled integral equations resulting from the resonatinggroup method, Bornapproximationis used. In this thesisthe quadratic aswell as the Cornell potential are used for pairwise interaction in the Hamiltonian of the four quark system. With the Cornell potential we incorporated the spin and flavour dependence in the total wave function of the four quark system. In this thesis a comparison of the cross sections obtained by using the quadratic potential and the Cornell potential is made. In this study we have found v that the Cornell potential gives lesser cross-sections as compared to the quadratic potential. We present the graphs which represent the justification of the difference of the cross sections ob tainedbytwodifferentpotentials. Inthisjustificationtheintegralkernelissplittedintotwoparts (i- potential part and ii- kinetic energy plus constant part). The results of these terms are plotted where it is observed that these terms try to cancel out each others effect to give the lesser hij factor which decreases the T matrix elements and hence the cross sections. This cancelation effect is large when Cornell potential is used. We then introduced the Gaussian form of f in the off diagonal parts of the kinetic energy, potential energy and the overlap matrices in the colour basis. There is a significant suppression in the cross sections obtained when f is introduced as compared to the cross sections obtained from simple sum of two body approach.
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