Star Formation Law at Sub-kpc Scale in the Elliptical Galaxy Centaurus A as Seen by ALMA

Abstract

We present an extensive analysis of the relationship between star formation rate surface density (∑SFR) and molecular gas surface density (∑[subscript]H2[/subscript] ) at sub-kpc scale in the elliptical galaxy Centaurus A (also known as NGC 5128) at the distance 3.8 Mpc. 12CO (J = 2-1) data from Atacama Large Millimetre/Sub-Millimetre Array SV data with very high resolution (2.9[variant prime][variant prime], 0.84[variant prime][variant prime]), as well as 24 μm data from the Spitzer Space Telescope, were used. This is one of the first studies of the SF law on Centaurus A at this very high spatial resolution. The results showed a breakdown in star formation law with a 0.49±0.05 index relating ∑SFR and ∑[subscript]H2[/subscript] at 185 pc. A significant correlation exists between surface densities of molecular gas and SFR with very long depletion time (68 Gy). In addition we examined the spatially resolved relationship between velocity dispersion and star formation rate surface density for the outer disk of this galaxy and we found that the average velocity dispersion is equal to 11.78 km/s. The velocity dispersion of the molecular ISM for the outer disk is found to follow a power relation with the star formation rate surface density σ[proportional, variant][superscript](∑SFR)β[/superscript] , where β is the slope from the ordinary least square fitting. The value of β is about 1/n[approximate]2.16±0.40 and n is the power law index of the star formation law.

Jazeel H. Azeez 1; 2 and Zamri Z. Abidin 1 and C.-Y. Hwang 3 and Zainol A. Ibrahim 1

Academic Editor:Dean Hines

1, Physics Department, Faculty of Science, University of Malaya, 50603 Kuala Lumpur, Malaysia

2, Physics Department, Faculty of Science, AL-Nahrain University, Baghdad 10072, Iraq

3, Graduate Institute of Astronomy, National Central University, Chung-Li 32054, Taiwan

Received 28 January 2017; Accepted 19 April 2017; 13 June 2017

This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction

The present challenge with elliptical galaxies is to resolve their formation and evolutionary history. Elliptical galaxies are currently known to contain an interstellar medium (ISM) that varies from that in a spiral galaxy [1]. Observations have previously detected cold gas, dust, and even new/residual star formation in elliptical galaxies [2-5]. It is well known that stars are formed from molecular gas, so studying the molecular gas in galaxies provides important indications of the primary physical process of massive star formation in galaxies [6]. The molecular gas in early-type galaxies was studied by many authors such as [7-10].

To understand star formation in galaxies, the relations between star formation rate surface density ∑SFR and gas surface density ∑gas must be determined. Schmidt [11] put forth a power law that presents a correlation between ∑SFR and ∑gas: ∑SFR[proportional, variant]^∑gasN . Kennicutt Jr. [12, 13] proved that the Schmidt law relates gas density to star formation density within many orders of magnitude and determined a power law relationship with index N=1.4. This relationship is usually called the Kennicutt-Schmidt (K-S) law. The most recent studies on the K-S law examined the index at sub-kpc scales [14-17], closing from the intrinsic scale of star formation, that is, giant molecular clouds size (GMCs) [6]. Kennicutt & Evans [18] reviewed the relation between the star formation at different scale from entire galaxies to individual molecular clouds; at sub-kiloparsec scale they recognized two regimes, the first with low density subthreshold regime and the second with high density regime. They found that the SFR density correlates well with the gas density for the second regime, while it is uncorrelated for the first one. The theories that describe and interpret the star formation process in these two regimes were studied by McKee & Ostriker [19].

One of the most interesting nearby galaxies is NGC 5128 (Centaurus A) (see [20], for a review of the properties of Cen A), the closest, most easily observable giant elliptical galaxy [21]. It is the dominant object in the Centaurus A group [22] and lies at a distance of 3.8 Mpc [23-25]. This distance (where 1[variant prime][variant prime] is approximately 18.5 pc) provides a unique opportunity to study the molecular gas in extraordinary detail. NGC 5128 shows considerably clear dust lanes that are probably caused by merger activities in the past (see [26, 27]). The molecular interstellar medium in the dust lane has been widely studied [28-36]. In addition, due to it being a strong source of radio and far infrared and X-ray emissions, it has been investigated in detail over a wide part of observable spectrum [37]. CO mapping reveals that the disk contains 2×¹⁰⁸ _M[ecedil]9; of molecular gas [29].

Rare studies covering the K-S law in Centaurus at sub-kpc scale have been reported. How do the SFR and H₂ surface densities relate to each other on sub-kpc spatial resolution in an elliptical galaxy? To address this question, we determine ∑_H2 in the central area of the elliptical galaxy Centaurus A by adopting high spatial resolution (185 pc).

2. Data

Observations of the Centaurus A in ¹² CO (J = 2-1) emission line were undertaken from August 11, 2011, at 19:19 (UTC) to August 12, 2011, at 01:00 (UTC) by using a mosaic of 48 pointing with a total integration time of ~341.5 min. These public data are available at the Atacama Large Millimetre/Submillimeter Array (ALMA) Science Portal (https://almascience.nrao.edu/alma-data/science-verification). Observations were conducted in band 6 (~1.3 mm). Four spectral windows were used, each with a 1.88 GHz bandwidth, 256 channels, and unique polarization. The data have a rms of 2.66 mJy with a spectral resolution of 20 km s^-1 . The observation parameters are listed in Table 1. The data were reduced, and images were processed using the Common Astronomy Software Application package (CASA). The continuum was first subtracted in the visibility domain. The images were processed using the CLEAN algorithm with a robust = 0.5 weighting (Briggs weighting) of the visibilities. The CO data were binned spectrally into channels with 20 km s^-1 wide. The procedure is described in the scripts available on the ALMA Science Portal (https://almascience.nrao.edu/almadata/sciver/CenABand6/).

Table 1: ALMA observational parameters.

Parameter	Value
Target	Centaurus A (CenA, NGC 5128)
Observing date	2011 August 11, 12
Total integration time	~341.5 min
Field center:
R.A. (J2000 )	1 2 h 2 5 m 27.6 1 s
Dec. (J2000 )	-43° 01[variant prime] 08.8[variant prime][variant prime]
Number of antenna	15
System velocity	542 ± 7 km s-1
Rest frequency	230 GHz
Restoring beam	(Major, minor, P.A.)
(2.9[variant prime][variant prime], 0.84[variant prime][variant prime], 82.65°)
Total bandwidth	1.88 GHz
Total channels	256
Velocity resolution	20 km s-1
Integrated flux density	6328.09 Jy km s-1
Redshift (z)	0.00183

To estimate the amount of star formation obscured by dust, we used 24 μ m data obtained by SPITZER (MIPS). The data was obtained from the public archive (http://sha.ipac.caltech.edu/applications/Spitzer/SHA/). The resolution element (beam size) of MIPS band is ~6[variant prime][variant prime], with pixel size of 2.55[variant prime][variant prime]. The 24 μ m data has a ~5[variant prime] square field of view.

3. Results and Discussion

3.1. CO Maps and Line Emission Distribution

The maps of the integrated intensity and velocity dispersion of the emission line ¹² CO (J = 2-1) are shown in Figures 1 and 2. We can see from Figure 1 that the distribution can be divided into three regions: a central emission region and two regions (northeast, NE, and southwest, SW, one on either side of the centre) forming an S-like shape. The NE region takes an arc shape that extends to the central region while the SW region takes a semiarc shape that extends from the central region and becomes fainter as it goes radially outwards. It is clear that the NE region is brighter than the SW region because the latter is CO poorer. These two regions have also been identified by Bland et al. [38], who observed ionized gas with Centaurus A. His results revealed that the HII regions were embedded in a faint component of diffusely ionized gas and confined to an envelope which has the form of a hysteresis loop. From the same figure it is noticed that the CO distribution is centrally peaked, and this is also observed in most Sc spiral galaxies [39, 40].

Figure 1: ALMA ¹² CO (J = 2-1) integrated intensity images of Centaurus A (NGC 5128).

[figure omitted; refer to PDF]

Figure 2: ALMA ¹² CO (J = 2-1) velocity dispersion images of Centaurus A (NGC 5128).

[figure omitted; refer to PDF]

3.2. Molecular Gas Mass and Surface Density

The mass of the molecular gas was calculated from the ¹² CO(2-1) emission line as tracer for molecular hydrogen gas using the following formula: [figure omitted; refer to PDF]

We adopt a CO(2-1)/CO(1-0) line ratio (_R21 ) of 0.55 [41]. The molecular hydrogen mass has been calculated in a region of (~1.5 kpc) diameter to be ~2 × 10⁸ _M[ecedil]9; by adopting the distance D = 3.8 Mpc. By comparing the data with the single dish [28] value of 1 × 10⁹ _M[ecedil]9; (with D = 7 Mpc), a difference of 33% is found by using the same distance. This difference is attributed to missing flux, because this data does not contain short spacing information (ACA and single dish), in addition the relatively short observation time and the high uncertainties in data calibration for the mentioned single dish may also participate in increasing the missing flux. In the present study, the central region of Centaurus A was divided into many boxes each one with angular resolutions of 10[variant prime][variant prime] × 10[variant prime][variant prime]. The angular to linear scale is 1[variant prime][variant prime] = 18.5 pc; thus, these boxes correspond to the 185 pc × 185 scale. In each box the molecular gas mass surface density was calculated using conversion factor _XCO = 2 × 10²⁰ cm^-2 (K km s^-1 )^-1 [42, 43]. The molecular gas mass and surface density of each region are listed in Table 2, which shows that some regions have huge amount of molecular gas mass (1-14 × 10⁶ _M[ecedil]9; ) this indicates that several GMC associations are located there [44].

Table 2: CO intensity, molecular gas density and mass, star formation rate, and star formation rate surface density. With spatial resolution of 185 pc × 185 pc.

Box	S C O ( 2 - 1 ) Δ V	M ( H 2 )	∑ H 2	SFR	∑ S F R
(Jy km s-1 )	M [ecedil]9; × 106	(M[ecedil]9; pc-2 )	(M[ecedil]9; yr-1 ) × 10-5	(M[ecedil]9; yr-1 kpc-2 ) × 10-3
1	14.82	0.76	22.29	2.57	0.75
2	16.47	0.85	24.77	2.76	0.81
3	10.81	0.56	16.25	2.29	0.67
4	14.43	0.74	21.70	2.07	0.60
5	9.22	0.47	13.86	2.03	0.59
6	26.91	1.38	40.46	3.59	1.05
7	74.44	3.83	111.93	4.18	1.22
8	25.01	1.29	37.61	3.64	1.06
9	19.79	1.02	29.75	2.54	0.74
10	16.87	0.87	25.37	2.24	0.65
11	22.13	1.14	33.27	2.48	0.72
12	68.81	3.54	103.46	4.63	1.35
13	77.83	4.01	117.03	5.42	1.58
14	38.03	1.96	57.18	4.22	1.23
15	25.97	1.34	39.05	2.73	0.80
16	27.73	1.43	41.69	2.61	0.76
17	66.21	3.41	99.55	3.85	1.12
18	97.44	5.01	146.50	5.63	1.64
19	91.71	4.72	137.89	4.91	1.43
20	31.03	1.60	46.66	2.93	0.85
21	40.32	2.08	60.63	3.40	0.99
22	145.17	7.47	218.27	5.88	1.72
23	202.96	10.44	305.17	6.81	1.99
24	64.85	3.34	97.50	3.25	0.95
25	22.44	1.15	33.74	2.38	0.69
26	38.45	1.98	57.81	2.73	0.80
27	174.01	8.95	261.64	5.01	1.46
28	110.14	5.67	165.60	4.92	1.44
29	76.56	3.94	115.11	3.93	1.15
30	71.07	3.66	106.86	2.56	0.75
31	36.16	1.86	54.37	2.58	0.75
32	170.50	8.77	256.36	4.91	1.44
33	64.95	3.34	97.65	4.72	1.38
34	59.27	3.05	89.12	6.75	1.97
35	38.24	1.97	57.50	3.14	0.92
36	118.58	6.10	178.29	3.52	1.03
37	113.87	5.86	171.21	5.16	1.51
38	86.84	4.47	130.57	9.61	2.81
39	73.34	3.77	110.27	8.03	2.35
40	32.85	1.69	49.39	2.79	0.82
41	15.31	0.79	23.02	2.60	0.76
42	60.13	3.09	90.40	3.45	1.01
43	290.90	14.97	437.38	10.97	3.20
44	178.02	9.16	267.67	67.35	19.68
45	79.69	4.10	119.82	6.51	1.90
46	40.40	2.08	60.74	2.85	0.83
47	40.85	2.10	61.42	3.47	1.01
48	90.88	4.68	136.64	10.99	3.21
49	228.49	11.76	343.54	7.74	2.26
50	45.07	2.32	67.77	4.79	1.40
51	22.76	1.17	34.23	2.54	0.74
52	74.14	3.82	111.47	5.67	1.66
53	147.76	7.60	222.17	6.43	1.88
54	27.92	1.44	41.98	3.46	1.01
55	36.12	1.86	54.31	4.08	1.19
56	182.48	9.39	274.37	5.63	1.64
57	49.71	2.56	74.74	3.54	1.04
58	92.37	4.75	138.89	4.67	1.37
59	103.44	5.32	155.53	5.84	1.71
60	47.43	2.44	71.32	4.17	1.22
61	19.06	0.98	28.66	2.84	0.83
62	50.73	2.61	76.28	4.29	1.25
63	115.24	5.93	173.27	5.95	1.74
64	65.64	3.38	98.69	5.83	1.70
65	36.63	1.88	55.08	3.57	1.04
66	14.23	0.73	21.39	2.54	0.74
67	53.09	2.73	79.82	4.12	1.20
68	85.09	4.38	127.93	5.41	1.58
69	95.66	4.92	143.84	6.73	1.97
70	28.83	1.48	43.35	3.74	1.09
71	30.92	1.59	46.49	2.74	0.80
72	37.06	1.91	55.73	3.73	1.09
73	58.65	3.02	88.18	4.30	1.26
74	24.50	1.26	36.83	3.17	0.93
75	16.90	0.87	25.40	2.04	0.60
76	20.26	1.04	30.45	2.32	0.68

Note . Column 1: region name. Column 2: intensity of ¹² CO (J = 2-1) emission. Column 3: molecular gas mass. Column 4: surface density of molecular hydrogen mass. Column 5: star formation rate. Column 6: Star formation rate surface density.

3.3. Star Formation Rate Surface Density and Star Formation Law

The infrared data are used as star formation tracers. The infrared data are obtained from the Spitzer Space Telescope. To estimate the amount of star formation obscured by dust, we use 24 μ m data obtained from the public archive which is taken with the MIPS instrument. According to Helou [45] and Eckart et al. [29] the Centaurus A has cirrus like colours; however, its effect is weak on our data due to two reasons; the first is the used wavelength is 24 μ m. Bendo et al. [46] made an overview of ancillary 24, 70, and 160 μ m data from the Multiband Imaging Photometer for Spitzer (MIPS) for samples of nearby galaxies (including Centaurus A). In their study they concluded that the cirrus like colour in Centaurus A and in the other galaxies is only effective at the wavelengths 70 and 160 μ m and its effect is not influential in 24 μ m. The second reason, as Eckart et al. [29] concluded, is that the cirrus clouds emission is due to cold dust with larger spatial extent than the molecular disk. In the current data we only focused on the molecular disk. Accordingly, the cirrus clouds emission outside the disk has no effect on the observed emission and as a result on star formation.

Wu et al. [47] showed that the SFR can be estimated from 24 μ m luminosity using the following formula: [figure omitted; refer to PDF] where _Lv is the 24 μ m dust luminosity. The archival 24 μ m data from MIPS show that there is very weak star formation (few 10^-5 -10^-4 _M[ecedil]9; yr^-1 ). The total SFR in this galaxy 3.89 × 10^-3 _M[ecedil]9; yr^-1 was found to be lower than the previous estimates. The relationship between the SFR and molecular gas surface densities which is known as star formation law or (Kennicutt-Schmidt law) is drawn for NGC 5128 with the spatial resolution of 10[variant prime][variant prime] × 10[variant prime][variant prime] as shown in Figure 3. The derived values of star formation rate surface density at this spatial resolution are shown in Table 2. ¹² CO (J = 2-1) was used as a molecular gas density indicator. All data points from the boxes at this spatial resolution were combined to fit a line in log-log space using ordinary least square fitting (solid line in Figure 3). We found a high significant correlation with correlation coefficient 0.75 with a probability p = 100%. The power law index of the ∑SFR-∑_H2 relation for the elliptical galaxy NGC 5128 data is about 0.49±0.05. This value is significantly lower than a typical power law index of the K-S law. In the Milky Way, young clusters are known to recede from their parents at a rate of 10 km s^-1 [48]. As they evolve, they recede from their parent GMCs by a scale of 100 pc over a time period of 10 Myr. The drift scale of 100 pc is close to our scale of 185 pc. This result indicates that the traditional K-S law in this elliptical galaxy holds at greater than 200 pc; thus, when the spatial resolution is below this value, the K-S law for this galaxy may be not valid. As proposed by Calzetti et al. [49] at such scales below 500 pc, the sampling effects are more clear than they are for larger scales. More thorough studies are needed to figure out the effect of sampling effects versus scales, especially for the high spatial resolution (small region size). In addition the type of fitting method has shown to have an effect on the results of star formation law as proved by Rahmani et al. [50], so it will be more worthy to try different fitting methods at high spatial resolutions. We also compared the CO masses with the SFR estimates in order to measure a star formation efficiency (depletion time). Using a conversion factor _XCO = 2 × 10²⁰ cm^-2 (K km s^-1 )^-1 led to long depletion time (68 Gyr), which indicates that the star formation is inefficient in this galaxy. It is clear that the depletion time of the molecular gas in this galaxy is longer than the Hubble time. This means a very low efficiency of forming stars. The efficiency may also depend on the pressure and the surface density of star (e.g., [51]), which is, on average, low in this galaxy. The solid red triangle in Figure 3 represents the nuclear region of Centaurus A. It is clear that the molecular gas at this point is obviously offset from the KS law, suggesting that this points is mainly affected by AGN activities instead of star formation [17]. This means that this point is powered by kinetic energy injection from the AGN jet/wind and leading to molecular gas reservoir not forming star efficiently [52].

Figure 3: Relation between the surface density of molecular hydrogen ∑_H2 and surface density of star formation rate ∑SFR. The solid line represents the linear square fit line.

[figure omitted; refer to PDF]

Figure 4 shows our elliptical galaxy, Centaurus A, and the normal spiral and starburst galaxies of Kennicutt [13] on the same plot for comparison. We then went on to investigate the position of Centaurus A on the Kennicutt-Schmidt (KS) relation. We found that this galaxy has comparable star formation surface densities to normal spiral galaxy centres, but it lies systematically offset from the KS relation, having lower star formation surface density. This is in agreement with Davis et al. [53] who compared the Kennicutt-Schmidt (KS) relation [13] of nearby spiral galaxies with that of the CO-detected ETGs. They found that the ETGs had lower average SFR surface densities at a given molecular gas surface density compared to spirals. This is in agreement with recent simulations by Martig et al. [54] who predicted a decrease in the SFEs of ETGs

Figure 4: Relation between the surface density of molecular gas ∑_H2 and ∑SFR for normal galaxies (blue squares), starburst galaxies (green triangle), and the elliptical galaxy Centaurus A (red circles). The gas surface density is derived from CO(2-1) emission. The normal and starburst galaxy samples are obtained from Kennicutt [13].

[figure omitted; refer to PDF]

As we know, the velocity dispersion of the gas is also an important parameter for the star formation law [55]. We present here a measurement of the velocity dispersion for molecular components of the ISM for the outer disk of Centaurus A. In Figure 5 we investigate the correlation of the velocity dispersion σ of molecular gas with the star formation rate surface density ∑SFR of the galaxy. The former one is estimated from the second moments map (Figure 2) of the galaxy using the data from ALMA. The velocity dispersion in outer disk ranges from 0.02 to 31.50 km/s with an average value of 11.78 km/s. This average value of velocity dispersion is consistent with previous measurements for the Milky Way [56], M33 [57], and other nearby galaxies [58-60]. We find a significant correlation coefficient r=0.59 with probability p = 99.99%. Generally the results indicate low values for the velocity dispersion. According to Krumholz & Dekel [61] the low velocity dispersion values are usually associated with low SFR values. The determined average value which is close to 10 indicates low star formation for this elliptical galaxy. This indicates that there is no gravitational collapse, accordingly there is no star formation. We can see from Figure 5 that the velocity dispersion of the molecular ISM for the outer disk follows a power relation σ[proportional, variant]^(∑SFR)β where β is the slope from the ordinary least square fitting. The value of β is found to be [approximate]1/n = 2.16±0.4 and n is the power low index of the star formation law. This power law correlation may be a natural consequence of the gas and star formation surface density scaling laws [62].

Figure 5: The velocity dispersion for each pixel σ of Centaurus A as a function of the SFR surface averaged (in units of _M[ecedil]9; /yr·kpc² ).

[figure omitted; refer to PDF]

4. Summary and Conclusions

We used a high spatial resolution mosaic of ALMA observations of the ¹² CO (J = 2-1) line emission as a molecular gas indicator in the central region of the elliptical galaxy Centaurus A (NGC 5128) at a distance of 3.8 Mpc (1[variant prime][variant prime] = 18.5 pc). We measured ∑SFR with 24 μ m data from the (MIPS) Spitzer Space Telescope. We investigated the SF law (SFL) for this elliptical galaxy at very high spatial resolution (185 pc), and the result showed a breakdown SFL at this spatial resolution. The best fit parameter for the star formation power law index is 0.49±0.05. The second moment map from ALMA data for this galaxy was used to find the velocity dispersion of the molecular component for the interstellar medium. The results for the average velocity dispersion are close to 10 kms^-1 which is associated with low star formation, due to no gravitational collapse, which leads to no star formation. This result is supported by the long depletion time (68 Gyr) (low star formation efficiency). In addition, we find a significant correlation between velocity dispersion for each pixel and star formation surface density which follows a power law relation σ[proportional, variant]^(∑SFR)β , where the value of β is approximately [approximate]1/n and n is set by the Kennicutt-Schmidt law ∑SFR[proportional, variant]^(∑gas)n . This power law correlation may be a natural result of the gas and star formation surface density scaling laws.

We can see that the star formation efficiency (SFE) is very low in this galaxy despite the fact that the amount of molecular gas reservoir available is huge when compared to standard star formation efficiencies. This suggests that some processes may prevent the star formation to proceed in the cold gas. These processes can be due to high kinetic energy injection from the AGN that suppress the star formation processes [44].

Acknowledgments

This paper makes use of the following ALMA data: ADS/JAO.ALMA#2011.0.00008.SV. ALMA is a partnership of ESO (representing its member states), NSF (USA), and NINS (Japan), together with NRC (Canada) and NSC and ASIAA (Taiwan), and KASI (Republic of Korea), in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated by ESO, AUI/NRAO, and NAOJ. The coauthor Zamri Z. Abidin would also like to acknowledge the University of Malaya's HIR Grant UM.S/625/3/HIR/28 for their funding.

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