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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59410 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{3}$ | 1.4388 | 1.631 | 0.8822 | [X:[1.3256], M:[0.9836, 0.9883], q:[0.4215, 0.4544], qb:[0.562, 0.5387], phi:[0.3372]] | [X:[[0, 6]], M:[[-1, 5], [0, 9]], q:[[-1, 10], [1, 0]], qb:[[0, -5], [0, 13]], phi:[[0, -3]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}$ | -3 | t^2.88 + 2*t^2.95 + t^2.97 + t^2.98 + t^3.89 + t^3.96 + t^3.98 + t^3.99 + t^4.06 + 2*t^4.9 + t^4.97 + 2*t^5. + t^5.07 + t^5.76 + 2*t^5.83 + t^5.85 + t^5.86 + 2*t^5.9 + 3*t^5.92 + 3*t^5.93 + t^5.94 + t^5.96 - 3*t^6. + t^6.01 - t^6.07 - t^6.1 + t^6.77 + t^6.83 + 3*t^6.84 + 2*t^6.86 + 2*t^6.87 + t^6.91 + 4*t^6.93 + 4*t^6.94 + 2*t^6.96 + t^6.97 - t^7.01 + 2*t^7.03 + t^7.04 - t^7.08 - t^7.11 + t^7.12 + 3*t^7.78 + 5*t^7.85 + 2*t^7.87 + 6*t^7.88 + t^7.92 + 6*t^7.95 + 2*t^7.97 + 3*t^7.98 + t^8.05 - t^8.12 + t^8.64 + 2*t^8.71 + t^8.73 + t^8.74 + 2*t^8.78 + 5*t^8.8 + 3*t^8.81 + t^8.83 + t^8.84 + 2*t^8.85 + 6*t^8.87 + t^8.88 + 8*t^8.9 + 3*t^8.91 + t^8.92 + t^8.94 - 8*t^8.95 + t^8.97 - 4*t^8.98 + 3*t^8.99 - t^4.01/y - t^5.02/y - t^6.89/y - (2*t^6.96)/y - t^6.98/y - t^6.99/y - t^7.9/y - (2*t^7.97)/y - t^7.99/y - t^8./y + (2*t^8.83)/y + t^8.85/y + t^8.86/y + t^8.9/y + t^8.92/y + (2*t^8.93)/y + t^8.94/y - t^8.99/y - t^4.01*y - t^5.02*y - t^6.89*y - 2*t^6.96*y - t^6.98*y - t^6.99*y - t^7.9*y - 2*t^7.97*y - t^7.99*y - t^8.*y + 2*t^8.83*y + t^8.85*y + t^8.86*y + t^8.9*y + t^8.92*y + 2*t^8.93*y + t^8.94*y - t^8.99*y | (g2^23*t^2.88)/g1 + (2*g2^5*t^2.95)/g1 + g2^9*t^2.97 + g1*g2^13*t^2.98 + (g2^20*t^3.89)/g1 + (g2^2*t^3.96)/g1 + g2^6*t^3.98 + g1*g2^10*t^3.99 + (g1*t^4.06)/g2^8 + (2*g2^17*t^4.9)/g1 + t^4.97/(g1*g2) + 2*g1*g2^7*t^5. + (g1*t^5.07)/g2^11 + (g2^46*t^5.76)/g1^2 + (2*g2^28*t^5.83)/g1^2 + (g2^32*t^5.85)/g1 + g2^36*t^5.86 + (2*g2^10*t^5.9)/g1^2 + (3*g2^14*t^5.92)/g1 + 3*g2^18*t^5.93 + g1*g2^22*t^5.94 + g1^2*g2^26*t^5.96 - 3*t^6. + g1*g2^4*t^6.01 - t^6.07/g2^18 - (g1^2*t^6.1)/g2^10 + (g2^43*t^6.77)/g1^2 + (g2^21*t^6.83)/g1^3 + (3*g2^25*t^6.84)/g1^2 + (2*g2^29*t^6.86)/g1 + 2*g2^33*t^6.87 + (g2^7*t^6.91)/g1^2 + (4*g2^11*t^6.93)/g1 + 4*g2^15*t^6.94 + 2*g1*g2^19*t^6.96 + g1^2*g2^23*t^6.97 - t^7.01/g2^3 + 2*g1*g2*t^7.03 + g1^2*g2^5*t^7.04 - t^7.08/g2^21 - (g1^2*t^7.11)/g2^13 + (g1^3*t^7.12)/g2^9 + (3*g2^40*t^7.78)/g1^2 + (5*g2^22*t^7.85)/g1^2 + (2*g2^26*t^7.87)/g1 + 6*g2^30*t^7.88 + (g2^4*t^7.92)/g1^2 + 6*g2^12*t^7.95 + 2*g1*g2^16*t^7.97 + 3*g1^2*g2^20*t^7.98 + g1^2*g2^2*t^8.05 - (g1^2*t^8.12)/g2^16 + (g2^69*t^8.64)/g1^3 + (2*g2^51*t^8.71)/g1^3 + (g2^55*t^8.73)/g1^2 + (g2^59*t^8.74)/g1 + (2*g2^33*t^8.78)/g1^3 + (5*g2^37*t^8.8)/g1^2 + (3*g2^41*t^8.81)/g1 + g2^45*t^8.83 + g1*g2^49*t^8.84 + (2*g2^15*t^8.85)/g1^3 + (6*g2^19*t^8.87)/g1^2 + (g2^23*t^8.88)/g1 + 8*g2^27*t^8.9 + 3*g1*g2^31*t^8.91 + g1^2*g2^35*t^8.92 + g1^3*g2^39*t^8.94 - (8*g2^5*t^8.95)/g1 + g2^9*t^8.97 - 4*g1*g2^13*t^8.98 + 3*g1^2*g2^17*t^8.99 - t^4.01/(g2^3*y) - t^5.02/(g2^6*y) - (g2^20*t^6.89)/(g1*y) - (2*g2^2*t^6.96)/(g1*y) - (g2^6*t^6.98)/y - (g1*g2^10*t^6.99)/y - (g2^17*t^7.9)/(g1*y) - (2*t^7.97)/(g1*g2*y) - (g2^3*t^7.99)/y - (g1*g2^7*t^8.)/y + (2*g2^28*t^8.83)/(g1^2*y) + (g2^32*t^8.85)/(g1*y) + (g2^36*t^8.86)/y + (g2^10*t^8.9)/(g1^2*y) + (g2^14*t^8.92)/(g1*y) + (2*g2^18*t^8.93)/y + (g1*g2^22*t^8.94)/y - t^8.99/(g1*g2^4*y) - (t^4.01*y)/g2^3 - (t^5.02*y)/g2^6 - (g2^20*t^6.89*y)/g1 - (2*g2^2*t^6.96*y)/g1 - g2^6*t^6.98*y - g1*g2^10*t^6.99*y - (g2^17*t^7.9*y)/g1 - (2*t^7.97*y)/(g1*g2) - g2^3*t^7.99*y - g1*g2^7*t^8.*y + (2*g2^28*t^8.83*y)/g1^2 + (g2^32*t^8.85*y)/g1 + g2^36*t^8.86*y + (g2^10*t^8.9*y)/g1^2 + (g2^14*t^8.92*y)/g1 + 2*g2^18*t^8.93*y + g1*g2^22*t^8.94*y - (t^8.99*y)/(g1*g2^4) |
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 |
---|---|---|---|---|---|---|---|---|---|
57574 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4383 | 1.6268 | 0.8841 | [X:[1.3334], M:[0.9834], q:[0.4279, 0.4611], qb:[0.5555, 0.5557], phi:[0.3333]] | 3*t^2.95 + t^3. + t^3.05 + 2*t^3.95 + t^4. + 2*t^4.05 + 3*t^4.95 + 3*t^5.05 + 5*t^5.9 + 4*t^5.95 - t^4./y - t^5./y - t^4.*y - t^5.*y | detail |