Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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58722 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ | 1.2015 | 1.4345 | 0.8375 | [X:[1.5701], M:[1.1402, 0.8598], q:[0.2149, 0.4954], qb:[0.2149, 0.4954], phi:[0.4299]] | [X:[[0, 1]], M:[[0, 2], [0, -2]], q:[[-1, 3], [-1, 7]], qb:[[1, -4], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}M_{1}M_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 3 | 2*t^2.13 + 2*t^2.58 + t^2.97 + 2*t^3.42 + 2*t^3.87 + 2*t^4.07 + 4*t^4.26 + 7*t^4.71 + 2*t^4.91 + 2*t^5.1 + t^5.16 + 2*t^5.36 + 7*t^5.55 + 2*t^5.8 + t^5.95 + 3*t^6. + 6*t^6.2 + 8*t^6.39 + 2*t^6.45 + 4*t^6.64 + 14*t^6.84 + 6*t^7.04 - 2*t^7.09 + 4*t^7.23 + 8*t^7.29 + 8*t^7.49 + 16*t^7.68 + t^7.74 + 2*t^7.88 + 2*t^7.93 + 2*t^8.08 + 12*t^8.13 + 16*t^8.33 + 2*t^8.38 + 16*t^8.52 - t^8.58 + 12*t^8.78 + t^8.92 + 26*t^8.97 - t^4.29/y - t^5.58/y - (2*t^6.42)/y - t^6.87/y + (3*t^7.71)/y + (2*t^8.1)/y - (2*t^8.16)/y + (3*t^8.55)/y - t^4.29*y - t^5.58*y - 2*t^6.42*y - t^6.87*y + 3*t^7.71*y + 2*t^8.1*y - 2*t^8.16*y + 3*t^8.55*y | 2*g2^3*t^2.13 + (2*t^2.58)/g2^2 + g2^7*t^2.97 + 2*g2^2*t^3.42 + (2*t^3.87)/g2^3 + (g1^3*t^4.07)/g2^9 + (g2^12*t^4.07)/g1^3 + 4*g2^6*t^4.26 + 7*g2*t^4.71 + (g1^3*t^4.91)/g2^5 + (g2^16*t^4.91)/g1^3 + 2*g2^10*t^5.1 + t^5.16/g2^4 + (g1^3*t^5.36)/g2^10 + (g2^11*t^5.36)/g1^3 + 7*g2^5*t^5.55 + (g1^3*t^5.8)/g2^15 + (g2^6*t^5.8)/g1^3 + g2^14*t^5.95 + 3*t^6. + (3*g1^3*t^6.2)/g2^6 + (3*g2^15*t^6.2)/g1^3 + 8*g2^9*t^6.39 + (2*t^6.45)/g2^5 + (2*g1^3*t^6.64)/g2^11 + (2*g2^10*t^6.64)/g1^3 + 14*g2^4*t^6.84 + (3*g1^3*t^7.04)/g2^2 + (3*g2^19*t^7.04)/g1^3 - (g1^3*t^7.09)/g2^16 - (g2^5*t^7.09)/g1^3 + 4*g2^13*t^7.23 + (8*t^7.29)/g2 + (4*g1^3*t^7.49)/g2^7 + (4*g2^14*t^7.49)/g1^3 + 16*g2^8*t^7.68 + t^7.74/g2^6 + g1^3*g2^2*t^7.88 + (g2^23*t^7.88)/g1^3 + (g1^3*t^7.93)/g2^12 + (g2^9*t^7.93)/g1^3 + 2*g2^17*t^8.08 + (g1^6*t^8.13)/g2^18 + 10*g2^3*t^8.13 + (g2^24*t^8.13)/g1^6 + (8*g1^3*t^8.33)/g2^3 + (8*g2^18*t^8.33)/g1^3 + (g1^3*t^8.38)/g2^17 + (g2^4*t^8.38)/g1^3 + 16*g2^12*t^8.52 - t^8.58/g2^2 + (6*g1^3*t^8.78)/g2^8 + (6*g2^13*t^8.78)/g1^3 + g2^21*t^8.92 + (g1^6*t^8.97)/g2^14 + 24*g2^7*t^8.97 + (g2^28*t^8.97)/g1^6 - t^4.29/(g2*y) - t^5.58/(g2^2*y) - (2*g2^2*t^6.42)/y - t^6.87/(g2^3*y) + (3*g2*t^7.71)/y + (2*g2^10*t^8.1)/y - (2*t^8.16)/(g2^4*y) + (3*g2^5*t^8.55)/y - (t^4.29*y)/g2 - (t^5.58*y)/g2^2 - 2*g2^2*t^6.42*y - (t^6.87*y)/g2^3 + 3*g2*t^7.71*y + 2*g2^10*t^8.1*y - (2*t^8.16*y)/g2^4 + 3*g2^5*t^8.55*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
57634 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$ | 1.5159 | 1.7675 | 0.8577 | [X:[], M:[0.6731, 0.6745], q:[0.4948, 0.4934], qb:[0.4948, 0.4934], phi:[0.3372]] | 3*t^2.02 + 3*t^2.96 + t^2.97 + t^3.04 + t^3.97 + t^3.98 + 3*t^4.04 + 3*t^4.05 + 6*t^4.98 + 10*t^4.99 + t^5.05 + 2*t^5.06 + 4*t^5.46 + t^5.92 + 8*t^5.93 + t^5.94 + t^5.99 + t^6. - t^4.01/y - t^5.02/y - t^4.01*y - t^5.02*y | detail |