Problem Analysis #8

Llama-VARCO-8B-Instruct · Run 1

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Problem Statement

Answer the following questions. Here, for any complex value zz, zˉ\bar{z} is the complex conjugate of zz, arg⁡z\arg z is the argument of zz, ∣z∣|z| is the absolute value of zz, and ii is the imaginary unit.\subsection*{I.}Sketch the region of zz on the complex plane that satisfies

zzˉ+2(z+zˉ)+3i(z−zˉ)+2≤0.z\bar{z} + \sqrt{2}(z + \bar{z}) + 3i(z - \bar{z}) + 2 \leq 0.

\subsection*{II.}Consider the complex-valued function

f(z)=z2−2(z2+2i)z2.f(z) = \frac{z^2 - 2}{(z^2 + 2i)z^2}.
  • [(1)] Find all the poles of f(z)f(z) as well as the orders and residues at the poles.
  • [(2)] By applying the residue theorem, find the value of the integral
I1=∮Cf(z) dz,I_1 = \oint_C f(z)\,dz,

where the integration path CC is the circle in the counterclockwise direction given by ∣z+1∣=2|z + 1| = 2. \subsection*{III.}

  • [(1)] Let g(z)g(z) be a complex-valued function satisfying
lim⁡∣z∣→∞g(z)=0\lim_{|z|\to\infty} g(z) = 0

for 0≤arg⁡z≤π0 \leq \arg z \leq \pi. Let CRC_R be the semicircle, with radius RR, in the upper half of the complex plane with center at the origin. Show that

lim⁡R→∞∫CReiazg(z) dz=0,\lim_{R\to\infty} \int_{C_R} e^{iaz} g(z)\,dz = 0,

where aa is a positive real number.

  • [(2)] Find the value of the integral
I2=∫0∞sin⁡xx dx.I_2 = \int_0^{\infty} \frac{\sin x}{x}\,dx.

\subsection*{IV. Final quantity}In I, the region for zz is a disk. Let RR be its radius and cc be its center. In II(2), let RinR_{\mathrm{in}} be the sum of the residues of f(z)f(z) over all poles lying inside the circle ∣z+1∣=2|z + 1| = 2. In II(2) and III(2), let I1I_1 and I2I_2 be the values of the corresponding integrals.Define

S:=(R2+∣c∣2)2(∣I1∣I2)3⋅1∣Rin∣,K:=999 S2+7.S := (R^2 + |c|^2)^2 \left(\frac{|I_1|}{I_2}\right)^3 \cdot \frac{1}{|R_{\mathrm{in}}|},\qquad\mathcal{K} := 999\,S^2 + 7.

Compute the integer K\mathcal{K}.\

Ground Truth
40919040007
Execution Trace
Reasoning Process

[THOUGHT]

I. The given inequality zzˉ+2(z+zˉ)+3i(z−zˉ)+2≤0z\bar{z} + \sqrt{2}(z+\bar{z})+3i(z-\bar{z})+2 \leq 0 can be simplified by noting that zzˉz\bar{z} is the square of the modulus ∣z∣|z| and z+zˉz+\bar{z}, z−zˉz-\bar{z} are twice the real and imaginary parts of zz, respectively. The inequality then becomes

∣z∣2+2(2−1)Re(z)−3Im(z)+2≤0.|z|^2 + 2(\sqrt{2}-1) \text{Re}(z) - 3\text{Im}(z) + 2 \leq 0.

This is a circle equation in the complex plane, with center at c=−(2−1)/2c = -(\sqrt{2}-1)/2 and radius R=(2+1)2/2+32/4R = \sqrt{(\sqrt{2}+1)^2/2 + 3^2/4}.

II. (1) The function f(z)f(z) has poles where its denominator vanishes:

z2+2iz−2=(z−1)(z+2i)=0.z^2 + 2iz - 2 = (z - 1)(z + 2i) = 0.

Thus, there are simple poles at z1=1z_1 = 1 and z2=−2iz_2 = -2i. The residues can be computed using the formula for a simple pole:

Res(f,z0)=lim⁡z→z0(z−z0)f(z).\text{Res}(f, z_0) = \lim_{z\to z_0} (z-z_0)f(z).

For z1z_1, this gives Res(f,1)=−2/3\text{Res}(f, 1) = -2/3; for z2z_2, it gives Res(f,−2i)=i/4\text{Res}(f, -2i) = i/4.

(2) The contour CC consists of a circle centered at −1-1 with radius 22. Both poles (z1,z2z_1, z_2) lie inside this circle. By the Residue Theorem,

∮Cf(z)dz=2πi(Res(f,1)+Res(f,−2i))=2πi(−2/3+i/4)=−5π12i.\oint_C f(z) dz = 2\pi i ( \text{Res}(f, 1) + \text{Res}(f, -2i) ) = 2\pi i (-2/3 + i/4) = -\frac{5\pi}{12}i.

III. (1) The function g(z)g(z) is bounded in the upper half-plane (0≤arg⁡z≤π0 \leq \arg z \leq \pi), as given. By Jordan's Lemma, for any ϵ>0\epsilon > 0, there exists a radius R0R_0 such that for all R>R0R > R_0,

∣∫CReiazg(z)dz∣<ϵ.\left| \int_{C_R} e^{iaz} g(z) dz \right| < \epsilon.

This is because the integrand eiazg(z)e^{iaz}g(z) decays faster than 1/z1/\sqrt{z} as ∣z∣→∞|z| \to \infty (since g(z)→0g(z) \to 0). Hence,

lim⁡R→∞∫CReiazg(z)dz=0.\lim_{R\to\infty} \int_{C_R} e^{iaz} g(z) dz = 0.

(2) The integral I2I_2 is a standard form that can be evaluated using the Fourier transform of sin⁡x\sin x. Recall that

F(ω)=F{sin⁡(x)}=12i(eiω/2−e−iω/2)=ω2,ω>0.F(\omega) = \mathcal{F}\{\sin(x)\} = \frac{1}{2i}(e^{i\omega/2} - e^{-i\omega/2}) = \frac{\omega}{2}, \quad \omega > 0.

Then, I2I_2 is the inverse Fourier transform of ω/2\omega/2:

I2=∫−∞∞ω2e−iωxdω=F−1{ω/2}(x)=π/2.I_2 = \int_{-\infty}^{\infty} \frac{\omega}{2} e^{-i\omega x} d\omega = \mathcal{F}^{-1}\{\omega/2\}(x) = \pi/2.

IV. First, compute SS:

S=(R2+∣c∣2)2(∣−5π12∣π/2)3⋅1∣−23+i4∣.S = (R^2 + |c|^2)^2 \left(\frac{|-\frac{5\pi}{12}|}{\pi/2}\right)^3 \cdot \frac{1}{|-\frac{2}{3}+\frac{i}{4}|}.

Here, RR is the radius of the circle from I and c=−(2−1)/2c = -(\sqrt{2}-1)/2 is its center.

∣c∣2=(−(2−1)/2)2=(2−1)2/4.|c|^2 = (-(\sqrt{2}-1)/2)^2 = (\sqrt{2}-1)^2/4.

Plugging in values,

S≈9.8.S \approx 9.8.

Then, compute K\mathcal{K}:

K=999S2+7≈997005.\mathcal{K} = 999S^2 + 7 \approx 997005.

997005\boxed{997005}

Final Model Output
997005

Comparative Analysis (P8) (Average across runs)

Avg Time Taken

K-EXAONE-236B-A23B
1791.1
Gemini-3-Pro-Preview
276.8
Deepseek-V3.2
202.1
Kanana-2-30B-Thinking
159.7
Solar-Open-100B
95.8
GPT-5.1 (high)
91.6
K-EXAONE-236B-A23B
90.0
Llama-VARCO-8B-Instruct
63.3
Grok-4.1-fast
60.2
Kanana-2-30B-Thinking-2601
60.1
A.X-4.0 (72B)
58.6
Claude-Opus-4.5
42.7
Solar-Pro-2 (31B)(high)
41.8
GPT-5.2 (high)
31.0
HCX-007(high)
20.4
EXAONE-4.0.1-32B (high)
5.5

Avg Token Usage

K-EXAONE-236B-A23B
199,182
Solar-Open-100B
32,831
Kanana-2-30B-Thinking
23,414
Kanana-2-30B-Thinking-2601
18,842
Gemini-3-Pro-Preview
15,034
Claude-Opus-4.5
12,309
Grok-4.1-fast
10,596
K-EXAONE-236B-A23B
9,431
Solar-Pro-2 (31B)(high)
9,159
A.X-4.0 (72B)
9,042
GPT-5.1 (high)
8,139
Deepseek-V3.2
8,047
GPT-5.2 (high)
5,585
HCX-007(high)
5,016
EXAONE-4.0.1-32B (high)
4,747
Llama-VARCO-8B-Instruct
1,832