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 |
|---|---|---|---|---|---|---|---|---|---|
| 61236 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4531 | 1.6405 | 0.8858 | [X:[1.3339], M:[1.0009, 1.0026, 0.9957], q:[0.4978, 0.503], qb:[0.4996, 0.5013], phi:[0.333]] | [X:[[0, 2]], M:[[0, 3], [0, 9], [0, -15]], q:[[-1, -3], [-1, 15]], qb:[[1, -6], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}$ | -3 | t^2.99 + 2*t^3. + 2*t^3.01 + t^3.99 + 2*t^4. + 2*t^4.01 + t^4.99 + t^5. + 2*t^5.01 + 2*t^5.5 + 2*t^5.51 + t^5.97 + 3*t^5.99 - 3*t^6. + 4*t^6.01 + 2*t^6.02 + t^6.49 + 2*t^6.5 + t^6.51 + t^6.98 + 4*t^6.99 + 5*t^7. + 6*t^7.01 + 2*t^7.02 + t^7.48 + t^7.49 + t^7.51 + t^7.52 + 2*t^7.98 + 5*t^7.99 + 7*t^8. + 6*t^8.01 + 4*t^8.02 - t^8.49 + t^8.5 + 3*t^8.51 + t^8.52 + t^8.96 + 3*t^8.98 + t^8.99 - t^4./y - t^5./y - t^6.99/y - (2*t^7.)/y - (2*t^7.01)/y - t^7.99/y - (2*t^8.)/y - (2*t^8.01)/y + t^8.98/y + t^8.99/y - t^4.*y - t^5.*y - t^6.99*y - 2*t^7.*y - 2*t^7.01*y - t^7.99*y - 2*t^8.*y - 2*t^8.01*y + t^8.98*y + t^8.99*y | t^2.99/g2^15 + t^3./g2^3 + g2^3*t^3. + 2*g2^9*t^3.01 + t^3.99/g2^10 + t^4./g2^4 + g2^2*t^4. + g2^8*t^4.01 + g2^14*t^4.01 + t^4.99/g2^11 + t^5./g2^5 + g2^7*t^5.01 + g2^13*t^5.01 + (g1^3*t^5.5)/g2^13 + (g2^8*t^5.5)/g1^3 + (g1^3*t^5.51)/g2^7 + (g2^26*t^5.51)/g1^3 + t^5.97/g2^30 + t^5.99/g2^12 + (2*t^5.99)/g2^6 - 3*t^6. + 2*g2^6*t^6.01 + 2*g2^12*t^6.01 + 2*g2^18*t^6.02 + (g2^7*t^6.49)/g1^3 + (g1^3*t^6.5)/g2^14 + (g1^3*t^6.5)/g2^8 + (g2^25*t^6.51)/g1^3 + t^6.98/g2^25 + (2*t^6.99)/g2^13 + (2*t^6.99)/g2^7 + (2*t^7.)/g2 + 3*g2^5*t^7. + 4*g2^11*t^7.01 + 2*g2^17*t^7.01 + 2*g2^23*t^7.02 + t^7.48/(g1^3*g2^12) + (g2^6*t^7.49)/g1^3 + (g1^3*t^7.5)/g2^15 + (g1^3*t^7.5)/g2^9 - (g2^12*t^7.5)/g1^3 - (g2^18*t^7.5)/g1^3 + (g2^24*t^7.51)/g1^3 + (g2^42*t^7.52)/g1^3 + t^7.98/g2^26 + t^7.98/g2^20 + (2*t^7.99)/g2^14 + (3*t^7.99)/g2^8 + (3*t^8.)/g2^2 + 4*g2^4*t^8. + 3*g2^10*t^8.01 + 3*g2^16*t^8.01 + 3*g2^22*t^8.02 + g2^28*t^8.02 - (g1^3*t^8.49)/g2^22 - t^8.49/(g1^3*g2) + (g2^5*t^8.49)/g1^3 + (g1^3*t^8.5)/g2^10 + (g1^3*t^8.51)/g2^4 + g1^3*g2^2*t^8.51 + (g2^23*t^8.51)/g1^3 + (g2^35*t^8.52)/g1^3 + t^8.96/g2^45 + t^8.98/g2^27 + (2*t^8.98)/g2^21 - t^8.99/g2^15 + (2*t^8.99)/g2^9 - t^4./(g2*y) - t^5./(g2^2*y) - t^6.99/(g2^16*y) - t^7./(g2^4*y) - (g2^2*t^7.)/y - (2*g2^8*t^7.01)/y - t^7.99/(g2^17*y) - t^8./(g2^5*y) - (g2*t^8.)/y - (2*g2^7*t^8.01)/y + t^8.98/(g2^18*y) + t^8.99/(g2^6*y) - (t^4.*y)/g2 - (t^5.*y)/g2^2 - (t^6.99*y)/g2^16 - (t^7.*y)/g2^4 - g2^2*t^7.*y - 2*g2^8*t^7.01*y - (t^7.99*y)/g2^17 - (t^8.*y)/g2^5 - g2*t^8.*y - 2*g2^7*t^8.01*y + (t^8.98*y)/g2^18 + (t^8.99*y)/g2^6 |
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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 59416 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ | 1.4756 | 1.6874 | 0.8745 | [X:[], M:[0.9923, 0.977], q:[0.5194, 0.4733], qb:[0.5036, 0.4882], phi:[0.3359]] | t^2.02 + t^2.88 + 2*t^2.93 + t^2.98 + t^3.02 + t^3.89 + t^3.94 + 2*t^4.03 + t^4.08 + 2*t^4.9 + 3*t^4.95 + t^4.99 + 2*t^5.04 + t^5.08 + t^5.41 + t^5.45 + t^5.49 + t^5.54 + t^5.77 + 2*t^5.82 + 3*t^5.86 + 4*t^5.91 + 3*t^5.95 - 3*t^6. - t^4.01/y - t^5.02/y - t^4.01*y - t^5.02*y | detail |